JPH1145416A - Magnetoresistance effect element and thin film magnetic head equipped with that element - Google Patents

Magnetoresistance effect element and thin film magnetic head equipped with that element

Info

Publication number
JPH1145416A
JPH1145416A JP12542498A JP12542498A JPH1145416A JP H1145416 A JPH1145416 A JP H1145416A JP 12542498 A JP12542498 A JP 12542498A JP 12542498 A JP12542498 A JP 12542498A JP H1145416 A JPH1145416 A JP H1145416A
Authority
JP
Japan
Prior art keywords
layer
length
magnetoresistance effect
ion milling
track width
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP12542498A
Other languages
Japanese (ja)
Inventor
Koichi Terunuma
幸一 照沼
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
TDK Corp
Original Assignee
TDK Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by TDK Corp filed Critical TDK Corp
Priority to JP12542498A priority Critical patent/JPH1145416A/en
Publication of JPH1145416A publication Critical patent/JPH1145416A/en
Pending legal-status Critical Current

Links

Abstract

PROBLEM TO BE SOLVED: To obtain a magnetoresistance effect layer in which the length of a tapered part formed on the end edge part of an opposite side to the surface facing to a magnetic medium on a magnetoresistance effect layer is properly stipulated by setting the conditions of ion milling so that the ratio of the length of the tapered part in the perpendicular direction to the track width direction to the length from the magnetoresistance effect layer to the end edge is a specified value or smaller. SOLUTION: A magnetoresistance effect (MR) layer 13 formed in a shield gap layer is formed as a strip shape in which a ferromagnetic body or a spin- bulb multilayered structure is extended in the track width direction. A tapered part 13a is formed on the end edge of the opposite side to a floating face 18 by ion milling treatment in the case of patterning the MR layer 13. The length L of the tapered part 13a is made so as to be <1/5 of the height hMR of the MR by controlling the conditions of ion milling. Thereby, decrease in an MR reproducing output and increase in the resistance of an MR element can be prevented and further, decrease in the presumed accuracy of the life of the MR element can be also prevented.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明は、磁気ディスク等の
磁気媒体上に記録されている情報を読出すための磁気抵
抗効果(MR)素子及びこのMR素子を備えた薄膜磁気
ヘッドに関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a magnetoresistive (MR) element for reading information recorded on a magnetic medium such as a magnetic disk and a thin film magnetic head provided with the MR element.

【0002】[0002]

【従来の技術】MR型薄膜磁気ヘッド(以下MRヘッド
と称する)におけるMR層は、一般に、NiFe等の強
磁性層を下部シールド層上に積層し、パターニングした
レジスト等のマスク上からイオンミリングを施すことに
よって形成される。
2. Description of the Related Art Generally, an MR layer in an MR type thin film magnetic head (hereinafter referred to as an MR head) is formed by laminating a ferromagnetic layer such as NiFe on a lower shield layer, and performing ion milling from a mask such as a patterned resist. It is formed by applying.

【0003】[0003]

【発明が解決しようとする課題】このように、MR層を
イオンミリングによってパターニングすると、磁気媒体
と対向する浮上面(ABS)とは反対側のその端縁の部
分が直角に終端せず、斜めに終端したテーパ部が形成さ
れてしまう。このテーパ部の長さL(トラック幅方向と
垂直の方向の長さ)が長くなると、MR層のABSとは
反対側の端縁を正確に規定できなくなり、MR層の高さ
MR(ABSの端縁からその反対側の端縁までの長さ、
以下MRハイトと称する)が正確に規定できなくなる。
また、MRハイトhMRが規定できたとしても、テーパ部
の長さLがこのMRハイトhMRに比して大きくなると、
MRヘッドの再生出力が低下し、MR素子としての抵抗
が大きくなり、しかもエレクトロマイグレーションによ
る寿命推定精度が低下してしまう。特に、このMRハイ
トは、記録密度が高くなってトラック幅が短くなると、
それに伴ってますます小さくする必要がある(MR層の
矩形形状のアスペクト比を一定に保つため)ため、テー
パ部の長さLの増大は大きな問題となる。
As described above, when the MR layer is patterned by ion milling, the edge portion on the side opposite to the air bearing surface (ABS) facing the magnetic medium does not end at a right angle but is inclined. End, a tapered portion is formed. If the length L (length in the direction perpendicular to the track width direction) of the tapered portion is increased, the edge of the MR layer opposite to the ABS cannot be accurately defined, and the height h MR (ABS Length from the edge of the to the opposite edge,
(Hereinafter referred to as MR height) cannot be accurately defined.
Further, even if the MR height h MR can be specified, if the length L of the tapered portion is larger than this MR height h MR ,
The reproduction output of the MR head decreases, the resistance as the MR element increases, and the accuracy of estimating the life due to electromigration decreases. In particular, when the recording density increases and the track width decreases,
Accordingly, it is necessary to further reduce the size (in order to keep the aspect ratio of the rectangular shape of the MR layer constant), so that the increase in the length L of the tapered portion becomes a serious problem.

【0004】従って本発明の目的は、MR層のテーパ部
の長さを適切に規定したMRヘッドを提供することにあ
る。
Accordingly, it is an object of the present invention to provide an MR head in which the length of the tapered portion of the MR layer is appropriately defined.

【0005】[0005]

【課題を解決するための手段】本発明によれば、トラッ
ク幅方向に伸長するストリップ形状のMR層を備えたM
R素子であって、このMR層の磁気媒体に対向する面と
は反対側の端縁の部分に形成されるテーパ部のトラック
幅方向と垂直の方向の長さ(L)を、MR層の上述した
面から端縁までの長さ(hMR)の約1/5以下に、好ま
しくは約1/10以下に設定したMR素子、及びこのM
R素子を備えたMRヘッドが提供される。なお、本発明
のMR素子は、異方性磁気抵抗効果(AMR)を利用し
たMR素子であってもよいし、スピンバルブ等の巨大磁
気抵抗効果(GMR)を利用したMR素子であってもよ
い。
According to the present invention, there is provided a magnetic head having a strip-shaped MR layer extending in a track width direction.
In the R element, the length (L) of the taper portion formed at the edge of the MR layer opposite to the surface facing the magnetic medium in the direction perpendicular to the track width direction (L) is defined as the length of the MR layer. An MR element set to about 1/5 or less, preferably about 1/10 or less of the length (h MR ) from the surface to the edge described above,
An MR head having an R element is provided. The MR element of the present invention may be an MR element utilizing the anisotropic magnetoresistance effect (AMR) or an MR element utilizing the giant magnetoresistance effect (GMR) such as a spin valve. Good.

【0006】形成されるMR層のL(テーパ部長さ)/
MR(MRハイト)が約1/5以下に、好ましくは約1
/10以下となるように、イオンミリング条件を設定す
る。テーパ部長さをこのように規定することにより、M
R再生出力の低下を防止でき、MR素子の抵抗増大を防
止できる。さらに、MR素子の寿命の推定精度の低下を
も防止できる。
L (length of tapered portion) of MR layer to be formed /
h MR (MR height) is about 1/5 or less, preferably about 1
The ion milling conditions are set so as to be / 10 or less. By defining the length of the tapered portion in this manner, M
A decrease in the R reproduction output can be prevented, and an increase in the resistance of the MR element can be prevented. Further, it is possible to prevent the accuracy of estimating the life of the MR element from being lowered.

【0007】[0007]

【発明の実施の形態】以下図面を用いて本発明の実施形
態を詳細に説明する。
Embodiments of the present invention will be described below in detail with reference to the drawings.

【0008】図1は本発明の一実施形態におけるMRヘ
ッドの層構成を概略的に示す断面図である。
FIG. 1 is a sectional view schematically showing a layer structure of an MR head according to an embodiment of the present invention.

【0009】同図において、10は下部シールド層、1
1は記録ヘッド側の下部磁極層をも兼用する上部シール
ド層、12は下部シールド層及び上部シールド層10及
び11間に挿設されたシールドギャップ層、13はシー
ルドギャップ層内に形成されたMR層、14は記録ギャ
ップ層、15は上部磁極層、16は絶縁層17内に設け
られたコイル、18は磁気媒体に対向する面である浮上
面(ABS)をそれぞれ示している。
In FIG. 1, reference numeral 10 denotes a lower shield layer;
Reference numeral 1 denotes an upper shield layer also serving as a lower magnetic pole layer on the recording head side, 12 denotes a shield gap layer inserted between the lower and upper shield layers 10 and 11, and 13 denotes an MR formed in the shield gap layer. Reference numeral 14 denotes a recording gap layer, 15 denotes an upper magnetic pole layer, 16 denotes a coil provided in an insulating layer 17, and 18 denotes an air bearing surface (ABS) facing the magnetic medium.

【0010】MR層13は、例えば、NiFe又はNi
FeCo等の強磁性体(AMRヘッドの場合)又はスピ
ンバルブ積層構造(GMRヘッドの場合)をトラック幅
方向に伸長するストリップ形状として形成したものであ
る。図2はこのMR層13の部分のみを拡大して表わし
た図である。同図からも明らかのように、MR層13を
パターニングする際のイオンミリング処理によって、こ
のMR層13のABS18とは反対側の端縁の部分にテ
ーパ部13aが形成されてしまう。
The MR layer 13 is made of, for example, NiFe or Ni
A ferromagnetic material such as FeCo (in the case of an AMR head) or a spin valve laminated structure (in the case of a GMR head) is formed in a strip shape extending in the track width direction. FIG. 2 is an enlarged view of only the MR layer 13. As is clear from the figure, the tapered portion 13a is formed at the edge of the MR layer 13 opposite to the ABS 18 due to the ion milling process when patterning the MR layer 13.

【0011】MRハイトhMRの方向のこのテーパ部13
aの長さLは、イオンビーム入射角度及びイオンミリン
グのためのレジスト等のマスクの厚さ等のイオンミリン
グ条件に応じて制御可能であることが分かった。このた
め、イオンミリング条件を変えて複数のMRヘッドを作
製し、MR素子抵抗を測定すると共にSEM(走査型電
子顕微鏡)を用いてMRハイトhMR及びテーパ部長さL
を測定した。
The tapered portion 13 in the direction of the MR height h MR
It has been found that the length L of a can be controlled in accordance with ion milling conditions such as the ion beam incident angle and the thickness of a mask such as a resist for ion milling. For this reason, a plurality of MR heads are manufactured by changing the ion milling conditions, the MR element resistance is measured, and the MR height h MR and the taper length L are measured using a scanning electron microscope (SEM).
Was measured.

【0012】図3はこの測定結果を示しており、横軸は
MR/L、縦軸はテーパ部13aが存在しない理想形状
である(L=0)として計算した素子抵抗(理想形状計
算値)に対する測定した素子抵抗(測定値)の増大割
合、即ち(測定値−理想形状計算値)/理想形状計算値
を表わしている。
FIG. 3 shows the measurement results, in which the horizontal axis represents h MR / L, and the vertical axis represents the element resistance (ideal shape calculated value) calculated on the assumption that the tapered portion 13a does not have an ideal shape (L = 0). ), The increase rate of the measured element resistance (measured value), that is, (measured value−calculated value of ideal shape) / calculated value of ideal shape.

【0013】同図から明らかのように、hMR/Lが約5
以上、好ましくは約10以上、即ちテーパ部長さLがM
RハイトhMRの約1/5以下、好ましくは約1/10以
下であれば、素子抵抗の増大割合が5%以下となり、実
際のMRヘッドとして問題ないレベルとなる。ちなみ
に、イオンビーム入射角度を約80度以上、好ましくは
90度(MR層の面に対して垂直)とし、マスクの厚さ
を約1.5μm以下、好ましくは約1.0μm以下とす
ることによって、hMR/Lは約10となる。従来のよう
に、マスクの厚さを約3.0μmとするとhMR/Lは約
3となり、この場合、素子抵抗の増大割合が約25%程
度と大きな値となってしまう。
As apparent from FIG. 1, h MR / L is about 5
Or more, preferably about 10 or more, that is, the length L of the tapered portion is M
If the R height h MR is about 1/5 or less, preferably about 1/10 or less, the increase rate of the element resistance becomes 5% or less, which is a level that does not cause a problem as an actual MR head. Incidentally, by setting the ion beam incident angle to about 80 degrees or more, preferably 90 degrees (perpendicular to the plane of the MR layer), and setting the thickness of the mask to about 1.5 μm or less, preferably about 1.0 μm or less. , H MR / L are about 10. As in the prior art, when the thickness of the mask is about 3.0 μm, h MR / L is about 3, and in this case, the increase rate of the element resistance is as large as about 25%.

【0014】本実施形態のようにhMR/Lを約5以上、
好ましくは約10以上とすることにより、MR素子の抵
抗増大を防止できる。さらに、MR再生出力の低下を防
止でき、MR素子の寿命の推定精度の低下をも防止でき
る。
As in the present embodiment, h MR / L is about 5 or more,
Preferably, the resistance is about 10 or more, so that an increase in resistance of the MR element can be prevented. Further, a decrease in the MR reproduction output can be prevented, and a decrease in the estimation accuracy of the life of the MR element can be prevented.

【0015】上述した実施形態では、MR層13のパタ
ーニングにイオンミリング処理を用いているが、その他
のエッチング処理、例えば反応性イオンエッチング(R
IE)処理を用いることも可能である。
In the above-described embodiment, the ion milling process is used for patterning the MR layer 13, but other etching processes, for example, reactive ion etching (R
It is also possible to use IE) processing.

【0016】以上述べた実施形態は全て本発明を例示的
に示すものであって限定的に示すものではなく、本発明
は他の種々の変形態様及び変更態様で実施することがで
きる。従って本発明の範囲は特許請求の範囲及びその均
等範囲によってのみ規定されるものである。
The embodiments described above are all illustrative of the present invention and not limiting, and the present invention can be embodied in other various modifications and alterations. Therefore, the scope of the present invention is defined only by the appended claims and their equivalents.

【0017】[0017]

【発明の効果】以上詳細に説明したように本発明によれ
ば、形成されるMR層のテーパ部長さL/MRハイトh
MRが約1/5以下、好ましくは約1/10以下となるよ
うに設定しているので、MR再生出力の低下を防止で
き、MR素子の抵抗増大を防止できる。さらに、MR素
子の寿命の推定精度の低下をも防止できる。
As described above in detail, according to the present invention, the length L / MR height h of the tapered portion of the formed MR layer.
Since the MR is set to be about 1/5 or less, preferably about 1/10 or less, a decrease in the MR reproduction output can be prevented, and an increase in the resistance of the MR element can be prevented. Further, it is possible to prevent the accuracy of estimating the life of the MR element from being lowered.

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

【図1】本発明の一実施形態におけるMRヘッドの層構
成を概略的に示す断面図である。
FIG. 1 is a sectional view schematically showing a layer configuration of an MR head according to an embodiment of the present invention.

【図2】図1のMR層の部分を拡大した図である。FIG. 2 is an enlarged view of a portion of an MR layer in FIG. 1;

【図3】hMR/Lと理想形状計算値に対する測定した素
子抵抗の増大割合との関係を示す図である。
FIG. 3 is a diagram showing a relationship between h MR / L and a measured increase rate of element resistance with respect to a calculated ideal shape.

【符号の説明】[Explanation of symbols]

10 下部シールド層 11 上部シールド層 12 シールドギャップ層 13 MR層 13a テーパ部 14 記録ギャップ層 15 上部磁極層 16 コイル 17 絶縁層 18 ABS DESCRIPTION OF SYMBOLS 10 Lower shield layer 11 Upper shield layer 12 Shield gap layer 13 MR layer 13a Tapered part 14 Recording gap layer 15 Upper pole layer 16 Coil 17 Insulating layer 18 ABS

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】 トラック幅方向に伸長するストリップ形
状の磁気抵抗効果層を備えた磁気抵抗効果素子であっ
て、該磁気抵抗効果層の磁気媒体に対向する面とは反対
側の端縁の部分に形成されるテーパ部の前記トラック幅
方向と垂直の方向の長さ(L)を、該磁気抵抗効果層の
前記面から前記端縁までの長さ(hMR)の約1/5以下
に設定したことを特徴とする磁気抵抗効果素子。
1. A magnetoresistive element including a strip-shaped magnetoresistive layer extending in a track width direction, wherein an end portion of the magnetoresistive layer opposite to a surface facing a magnetic medium is provided. The length (L) of the tapered portion formed in the direction perpendicular to the track width direction to about 1/5 or less of the length (h MR ) from the surface of the magnetoresistive layer to the edge. A magnetoresistive effect element characterized by being set.
【請求項2】 前記磁気抵抗効果層の磁気媒体に対向す
る面とは反対側の端縁の部分に形成されるテーパ部の前
記トラック幅方向と垂直の方向の長さ(L)を、該磁気
抵抗効果層の前記面から前記端縁までの長さ(hMR)の
約1/10以下に設定したことを特徴とする請求項1に
記載の磁気抵抗効果素子。
2. A length (L) of a taper portion formed at an end portion of the magnetoresistive layer opposite to a surface facing a magnetic medium in a direction perpendicular to the track width direction. 2. The magnetoresistive element according to claim 1, wherein the length (h MR ) from said surface of said magnetoresistive layer to said edge is set to about 1/10 or less.
【請求項3】 請求項1又は2に記載の磁気抵抗効果素
子を備えたことを特徴とする薄膜磁気ヘッド。
3. A thin film magnetic head comprising the magnetoresistive element according to claim 1.
JP12542498A 1997-05-29 1998-04-21 Magnetoresistance effect element and thin film magnetic head equipped with that element Pending JPH1145416A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP12542498A JPH1145416A (en) 1997-05-29 1998-04-21 Magnetoresistance effect element and thin film magnetic head equipped with that element

Applications Claiming Priority (3)

Application Number Priority Date Filing Date Title
JP9-154362 1997-05-29
JP15436297 1997-05-29
JP12542498A JPH1145416A (en) 1997-05-29 1998-04-21 Magnetoresistance effect element and thin film magnetic head equipped with that element

Publications (1)

Publication Number Publication Date
JPH1145416A true JPH1145416A (en) 1999-02-16

Family

ID=26461865

Family Applications (1)

Application Number Title Priority Date Filing Date
JP12542498A Pending JPH1145416A (en) 1997-05-29 1998-04-21 Magnetoresistance effect element and thin film magnetic head equipped with that element

Country Status (1)

Country Link
JP (1) JPH1145416A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2007243204A (en) * 2007-04-09 2007-09-20 Yamaha Corp Magnetic sensor

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2007243204A (en) * 2007-04-09 2007-09-20 Yamaha Corp Magnetic sensor
JP4640370B2 (en) * 2007-04-09 2011-03-02 ヤマハ株式会社 Magnetic sensor

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