JP2798016B2 - Magnetoresistive element, magnetoresistive head and method of manufacturing the same - Google Patents
Magnetoresistive element, magnetoresistive head and method of manufacturing the sameInfo
- Publication number
- JP2798016B2 JP2798016B2 JP7241572A JP24157295A JP2798016B2 JP 2798016 B2 JP2798016 B2 JP 2798016B2 JP 7241572 A JP7241572 A JP 7241572A JP 24157295 A JP24157295 A JP 24157295A JP 2798016 B2 JP2798016 B2 JP 2798016B2
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- film
- permanent magnet
- magnetoresistive
- flux density
- 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.)
- Expired - Fee Related
Links
- 238000004519 manufacturing process Methods 0.000 title claims description 11
- 230000004907 flux Effects 0.000 claims description 28
- 230000005415 magnetization Effects 0.000 claims description 28
- 230000000694 effects Effects 0.000 claims description 20
- 230000005381 magnetic domain Effects 0.000 claims description 11
- 230000001747 exhibiting effect Effects 0.000 claims description 4
- 238000005259 measurement Methods 0.000 claims description 2
- 238000010586 diagram Methods 0.000 description 14
- 230000005330 Barkhausen effect Effects 0.000 description 12
- 238000000034 method Methods 0.000 description 8
- 230000035945 sensitivity Effects 0.000 description 5
- 230000006641 stabilisation Effects 0.000 description 4
- 238000011105 stabilization Methods 0.000 description 4
- 229910001030 Iron–nickel alloy Inorganic materials 0.000 description 3
- 238000001514 detection method Methods 0.000 description 3
- 239000000956 alloy Substances 0.000 description 2
- 229910045601 alloy Inorganic materials 0.000 description 2
- 230000007423 decrease Effects 0.000 description 2
- 230000000087 stabilizing effect Effects 0.000 description 2
- 101150109831 SIN4 gene Proteins 0.000 description 1
- 239000002131 composite material Substances 0.000 description 1
- 230000002950 deficient Effects 0.000 description 1
- 230000002349 favourable effect Effects 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 238000004544 sputter deposition Methods 0.000 description 1
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- Magnetic Heads (AREA)
- Hall/Mr Elements (AREA)
Description
【0001】[0001]
【発明の属する技術分野】本発明は、磁気抵抗効果素
子、磁気抵抗型磁気ヘッド及びその製造方法に関し、さ
らに詳細に述べれば、永久磁石膜で磁化安定を行って磁
気的雑音を低減する磁気抵抗効果型感磁素子において、
製造歩留まりを向上する素子構造に関するものである。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a magnetoresistive element, a magnetoresistive magnetic head and a method of manufacturing the same, and more particularly, to a magnetoresistive element for stabilizing magnetization with a permanent magnet film to reduce magnetic noise. In the effect type magnetic sensing element,
The present invention relates to an element structure for improving a manufacturing yield.
【0002】[0002]
【従来の技術】近年の磁気記録の高密度化の進展に伴
い、その記録再生に用いる磁気ヘッドとして、磁気抵抗
効果型磁気ヘッド(以下MRヘッドと略称する)が実用
に供されるようになってきた。このMRヘッドの形状
は、一般に図5に示すように、磁気抵抗効果を示す磁性
膜の感磁部1と、感磁部1にセンス電流Jを印加するセ
ンス電流印加手段(電流源)Iと、感磁部1の電気抵抗
変化を検出する感磁部抵抗検出手段(電圧計測部)Vと
から成っている。また、感磁部1の構造は、図6に示す
ように、磁気抵抗効果膜(以下、MR膜と略称する)1
1と非磁性膜12及びMR膜11に適当なバイアス磁化
を付与する隣接軟磁性膜(以下、Soft Adjacent Layer;
SAL膜と略称する)13とから成る。2. Description of the Related Art With the recent development of high density magnetic recording, a magnetoresistive head (hereinafter abbreviated as MR head) has come into practical use as a magnetic head used for recording and reproduction. Have been. The shape of the MR head is generally as shown in FIG. 5, the magnetic sensitive section 1 of the magnetic film exhibiting magnetoresistance effect, the sense current applying means for indicia pressurizing the sensing current J in sensitive sections 1 (current source) I And a magnetic sensing unit resistance detecting means (voltage measuring unit) V for detecting a change in electric resistance of the magnetic sensing unit 1. Further, as shown in FIG. 6, the structure of the magnetic sensing unit 1 is a magnetoresistive film (hereinafter abbreviated as MR film) 1.
1 and an adjacent soft magnetic film (hereinafter referred to as Soft Adjacent Layer;
SAL film 13).
【0003】通常は、外部磁界Hに対する抵抗変化の直
線性を確保するために、MR膜の印加電流Jに対する磁
化の角度αをおよそ45゜に設定する。このとき、MR
膜11の飽和磁束密度及び膜厚を各々Bm ,tm とし、
SAL膜13の飽和磁束密度及び膜厚を各々Bs ,ts
とすると、SAL膜13の飽和磁束密度と膜厚との積
(Bs ・ts )は、あらかじめ(Bm ・tm )sin4
5゜にほぼ等しくなるように設定される。Normally, in order to ensure the linearity of the resistance change with respect to the external magnetic field H, the angle α of magnetization with respect to the applied current J of the MR film is set to about 45 °. At this time, MR
Let the saturation magnetic flux density and the film thickness of the film 11 be B m and t m , respectively.
The saturation magnetic flux density and the film thickness of the SAL film 13 are set to B s and t s respectively.
When the product of the saturation magnetic flux density and the film thickness of the SAL film 13 (B s · t s) in advance (B m · t m) sin4
It is set to be approximately equal to 5 °.
【0004】しかしながら、このような条件に設定して
も、図7の抵抗−磁界応答曲線に示すように、感磁部1
のMR膜11が特定の磁界で急激に抵抗変化を生じる現
象がしばしば見られた。このようなMR膜11の抵抗の
急激な変化を生じる現象をバルクハウゼンノイズとい
う。このバルクハウゼンノイズの発生原因は、MR膜1
1内に磁区が存在し、その磁区の境界である磁壁が急激
に移動することによるものである。However, even when such conditions are set, as shown in the resistance-magnetic field response curve of FIG.
The phenomenon that the MR film 11 rapidly changes its resistance by a specific magnetic field was often observed. Such a phenomenon that causes a rapid change in the resistance of the MR film 11 is called Barkhausen noise. The cause of the Barkhausen noise is that the MR film 1
This is due to the existence of a magnetic domain in 1 and the abrupt movement of the domain wall which is the boundary of the magnetic domain.
【0005】この磁壁の急激な移動を低減する方法とし
ては、図5及び図6に示すように、感磁部1の両側に永
久磁石膜2を設け、永久磁石膜2から発生する磁界によ
り感磁部1のMR膜11を単磁区化することが一般的に
行われている。この場合の条件として、永久磁石膜2の
飽和磁束密度及び膜厚を各々Bh ,th とすると、磁束
の連続性を良好に保つためには、永久磁石膜2の飽和磁
束密度と膜厚との積(Bh ・th )を(Bm ・tm )c
os45゜に等しくすることが必要となる。そうする
と、図8に示すような良好なMR抵抗−磁界応答曲線が
得られ、MRヘッドとして望ましい応答曲線になる。As a method for reducing the rapid movement of the magnetic domain wall, as shown in FIGS. 5 and 6, permanent magnet films 2 are provided on both sides of a magnetic sensing portion 1 so that the magnetic field generated by the permanent magnet film 2 can be used. It is common practice to make the MR film 11 of the magnetic part 1 into a single magnetic domain. In this case, assuming that the saturation magnetic flux density and the film thickness of the permanent magnet film 2 are B h and t h , respectively, the saturation magnetic flux density and the film thickness of the permanent magnet film 2 are required to maintain good continuity of magnetic flux. The product (B h · t h ) with (B m · t m ) c
os45 °. Then, a favorable MR resistance-magnetic field response curve as shown in FIG. 8 is obtained, and the response curve becomes desirable as an MR head.
【0006】[0006]
【発明が解決しようとする課題】次に、再現性よくバル
クハウゼンノイズを防止するには、永久磁石膜の飽和磁
束密度及び膜厚を精度よく制御することが必要である。
この永久磁石膜の飽和磁束密度と膜厚は、MRヘッドの
製造工程中で設定する。バルクハウゼンノイズの発生の
有無は、少なくともMRヘッドの素子が形成した後でな
ければ確認できない。従って、その時点でバルクハウゼ
ンノイズの存在が確認されれば、そのMRヘッドの素子
ウェーハは不良とせざるを得ない。Next, in order to prevent Barkhausen noise with good reproducibility, it is necessary to precisely control the saturation magnetic flux density and the film thickness of the permanent magnet film.
The saturation magnetic flux density and the film thickness of the permanent magnet film are set during the manufacturing process of the MR head. The presence or absence of Barkhausen noise cannot be confirmed until at least after the elements of the MR head are formed. Therefore, if the existence of Barkhausen noise is confirmed at that time, the element wafer of the MR head must be defective.
【0007】すなわち、バルクハウゼンノイズの修正を
行なうには、既に完了した永久磁石膜の特性を変更する
必要があるが、一般にはこれは、製造プロセス上極めて
困難である。すなわち、従来の永久磁石バイアス型のM
Rヘッドでは、歩留まりを向上し、かつ製造コストを低
減するのは困難であった。That is, in order to correct Barkhausen noise, it is necessary to change the characteristics of the completed permanent magnet film, but this is generally extremely difficult in the manufacturing process. That is, the conventional permanent magnet bias type M
With the R head, it has been difficult to improve the yield and reduce the manufacturing cost.
【0008】また、バルクハウゼンノイズを抑制する方
法として、永久磁石膜から発生する磁界を充分に強くす
ることも効果的ではあるが、発生磁界を強くすると、図
8に示す抵抗−磁界応答曲線の半値幅が拡がり、磁界検
出感度が低下するという欠点がある。As a method of suppressing Barkhausen noise, it is effective to sufficiently increase the magnetic field generated from the permanent magnet film. However, when the generated magnetic field is increased, the resistance-magnetic field response curve shown in FIG. There is a drawback that the half width is increased and the magnetic field detection sensitivity is reduced.
【0009】[0009]
【課題を解決するための手段】本発明のMR素子は、磁
気抵抗効果を示す磁性膜で形成される感磁部と、この感
磁部に印加されるセンス電流と、感磁部の両側に設けた
永久磁石膜で形成される磁区安定パタンとを有するMR
素子において、磁区安定パタンの磁化方向とセンス電流
の印加方向とが実質的に非平行であることを特徴とす
る。According to the MR element of the present invention, a magnetically sensitive portion formed of a magnetic film exhibiting a magnetoresistive effect, a sense current applied to the magnetically sensitive portion, and two sides of the magnetically sensitive portion are provided. Having magnetic domain stabilization pattern formed by provided permanent magnet film
The device is characterized in that the direction of magnetization of the magnetic domain stabilization pattern and the direction of application of the sense current are substantially non-parallel.
【0010】また、感磁部の磁性膜の飽和磁束密度及び
膜厚を各々Bm ,tm 、磁性膜の磁化方向とセンス電流
の印加方向とのなす角をα、センス電流の印加方向と永
久磁石膜の磁化方向とのなす角をθ、永久磁石膜の飽和
磁束密度及び膜厚を各々Bh,th とするとき、 (Bm ・tm )cosα≧(Bh ・th )cosθ を満たすように、前記θを定めてもよく、感磁部の磁性
膜の飽和磁束密度及び膜厚を各々Bm ,tm 、磁性膜の
磁化方向と前記センス電流の印加方向とのなす角αがほ
ぼ45°、永久磁石膜の飽和磁束密度及び膜厚を各々B
h ,th とするとき、 (Bm ・tm )cosα<(Bh ・th ) を満たすようにしてもよい。Also, the saturation magnetic flux density and the thickness of the magnetic film of the magnetic sensing portion are B m and t m , respectively, the angle between the magnetization direction of the magnetic film and the sense current application direction is α, and the sense current application direction is the angle between the magnetization direction of the permanent magnet film theta, each B h a saturation magnetic flux density and the film thickness of the permanent magnet film, when a t h, (B m · t m) cosα ≧ (B h · t h) The above θ may be determined so as to satisfy cos θ. The saturation magnetic flux density and the film thickness of the magnetic film of the magnetic sensing portion are respectively B m and t m , and the magnetization direction of the magnetic film and the direction of application of the sense current are formed. The angle α is approximately 45 °, and the saturation magnetic flux density and the film thickness of the permanent magnet film are respectively B
When h and t h , (B m · t m ) cosα <(B h · th h ) may be satisfied.
【0011】さらに、本発明のMRヘッドは、これらの
MR素子と、このMR素子を膜厚方向に両側から磁気シ
ールドとを備えることを特徴とする。Further, the MR head according to the present invention is characterized in that the MR head is provided with these MR elements and magnetic shields from both sides in the film thickness direction.
【0012】また、本発明のMRヘッド製造方法は、M
R素子に交流磁界を印加しながらMR素子の抵抗−磁界
応答を測定し、かつこの測定結果に基づいてMR素子の
永久磁石膜の着磁方向を任意に変更し、永久磁石膜の磁
化方向を最適化するようにしたことを特徴とする。Further, the method of manufacturing an MR head of the present invention
The resistance-magnetic field response of the MR element is measured while applying an AC magnetic field to the R element, and the magnetization direction of the permanent magnet film of the MR element is arbitrarily changed based on the measurement result to change the magnetization direction of the permanent magnet film. It is characterized by being optimized.
【0013】このように、本発明は、磁気抵抗効果を示
す磁性膜で形成される感磁部と、この感磁部に印加され
るセンス電流と、感磁部の両側に設けた永久磁石膜で形
成される磁区安定パタンを有するMR素子において、磁
区安定パタンの磁化方向が、センス電流印加方向と実質
的に非平行に設定し、その非平行の角度をMR素子形成
後に変化させることにより、磁界検出感度の低下を招く
ことなくバルクハウゼンノイズを抑制する。As described above, the present invention provides a magnetic sensing portion formed of a magnetic film exhibiting a magnetoresistive effect, a sense current applied to the magnetic sensing portion, and a permanent magnet film provided on both sides of the magnetic sensing portion. In the MR element having the magnetic domain stabilization pattern formed by the above, by setting the magnetization direction of the magnetic domain stabilization pattern substantially non-parallel to the sense current application direction, and changing the non-parallel angle after the MR element is formed, Barkhausen noise is suppressed without lowering the magnetic field detection sensitivity.
【0014】[0014]
【発明の実施の形態】次に、本発明について図面を参照
して説明する。 (第1の実施の形態)図1は、本発明の第1の実施の形
態を示す構成図である。図1を参照すると、第1の実施
の形態は、飽和磁束密度Bm ,膜厚tm を持つMR膜で
形成される感磁部1の両側に永久磁石膜2を配置する。
また、永久磁石膜2には、それぞれセンス電流印加手段
(電流源)Iと感磁部抵抗測定手段(電圧計測部)Vと
が接続されている。そして、符号15は感磁部1の磁化
方向、符号Jは感磁部1のMR膜(図示せず)に印加さ
れるセンス電流の方向、符号25は永久磁石膜2の磁化
方向をそれぞれ示している。Next, the present invention will be described with reference to the drawings. (First Embodiment) FIG. 1 is a configuration diagram showing a first embodiment of the present invention. Referring to FIG. 1, in the first embodiment, permanent magnet films 2 are arranged on both sides of a magnetosensitive portion 1 formed of an MR film having a saturation magnetic flux density Bm and a film thickness tm.
Further, a sense current applying means (current source) I and a magneto-sensitive section resistance measuring means (voltage measuring section) V are connected to the permanent magnet film 2 respectively. Reference numeral 15 denotes the magnetization direction of the magnetic sensing unit 1, reference numeral J denotes the direction of the sense current applied to the MR film (not shown) of the magnetic sensing unit 1, and reference numeral 25 denotes the magnetization direction of the permanent magnet film 2. ing.
【0015】ここで、永久磁石膜2の飽和磁束密度
Bh ,膜厚th は、その積が成膜工程の公差や余裕度を
考慮し、あらかじめ (Bm ・tm )cos45°<(Bh ・th ) ……………… (1) となるように設定しておく。また、大きさについては特
に厳しい制限は必要がない。従って、成膜工程中では飽
和磁束密度,膜厚についての厳しい制御を行なう必要が
ないため、工程の歩留りは向上する。 (第2の実施の形態)図2は、本発明の第2の実施の形
態を示す構成図である。図2を参照すると、第2の実施
の形態では、感磁部1のMR膜の印加センス電流Jと磁
化15とのなす角度をαとする。この角度αは、例え
ば、図8に示すように、抵抗−磁界応答曲線において最
適のバイアスが得れれるように、ほぼ45°に設定す
る。そして、この設定には、図3に示すSAL13の飽
和磁束密度Bs と膜厚ts との積を、あらかじめ、MR
膜の飽和磁束密度Bm と膜厚tm との積のsinα≒s
in45°=2-1/2倍とする。すなわち、 (Bs ・ts )≒(Bm ・tm )sin45° ……………… (2) となる。Here, the product of the saturation magnetic flux density B h and the thickness t h of the permanent magnet film 2 is determined in advance in consideration of the tolerance and the allowance of the film forming process, and (B m · t m ) cos 45 ° <( B h・ th h ) ……………… (1) In addition, there is no particular strict restriction on the size. Therefore, it is not necessary to strictly control the saturation magnetic flux density and the film thickness during the film forming process, and the process yield is improved. (Second Embodiment) FIG. 2 is a configuration diagram showing a second embodiment of the present invention. Referring to FIG. 2, in the second embodiment, the angle between the sense current J applied to the MR film of the magnetosensitive portion 1 and the magnetization 15 is α. The angle α is set to approximately 45 °, for example, as shown in FIG. 8, so that an optimum bias can be obtained in the resistance-magnetic field response curve. Then, this setting, the product of the saturation flux density B s and the thickness t s of SAL13 shown in FIG. 3, in advance, MR
Sinα ≒ s of the product of the saturation magnetic flux density B m of the film and the film thickness t m
in 45 ° = 2 -1/2 times. That is, the (B s · t s) ≒ (B m · t m) sin45 ° .................. (2).
【0016】また、永久磁石膜2については、この永久
磁石膜2の飽和磁束密度及び膜厚を各々Bh ,th とし
たとき、飽和磁束密度Bh と膜厚th との積を(Bm ・
tm)cos45°よりも余裕を持って大きく設定して
いる。従って、このまま、永久磁石膜2の磁化方向25
をセンス電流方向Jと同じ向きに設定するすると、余分
な磁束が発生し、感磁部1に不必要な磁界が電流方向に
加わり、図8に示す磁界−抵抗曲線の半値幅が増大して
感磁感度が低下する。Further, for the permanent magnet film 2, each B h a saturation magnetic flux density and the film thickness of the permanent magnet film 2, when a t h, the product of the saturation flux density B h and the thickness t h ( B m・
t m ) is set to be larger than cos 45 ° with a margin. Therefore, the magnetization direction 25 of the permanent magnet film 2 remains unchanged.
Is set in the same direction as the sense current direction J, an extra magnetic flux is generated, an unnecessary magnetic field is applied to the magnetosensitive portion 1 in the current direction, and the half value width of the magnetic field-resistance curve shown in FIG. The magnetic sensitivity decreases.
【0017】この感磁感度の低下を抑制するには、感磁
部のMR膜のセンス電流方向の磁束と、永久磁石膜の同
方向の磁束が等しくなるように、永久磁石膜の磁化25
の方向を設定する。すなわち、永久磁石膜の磁化方向を
θとすると、 (Bh ・th )cosθ≒(Bm ・tm )cos45° …… (3) にθを設定している。 (第3の実施の形態)図4は、本発明の第3の実施の形
態を示す構成図である。図4を参照すると、第3の実施
の形態は、MR素子の具体的な材料構成に関するもので
ある。MR膜11はNiFe膜から成り、Bm ≒850
0G,tm ≒20nmである。また、非磁性膜12には
膜厚10nmのTa膜を用いる。さらに、SAL膜13
は非晶質CoZrMo膜から成り、飽和磁束密度Bs ≒
6000G,膜厚ts ≒20nmである。この場合は条
件式(2) を満足している。In order to suppress the decrease in the magnetic sensitivity, the magnetization of the permanent magnet film is set so that the magnetic flux in the sense current direction of the MR film of the magnetic sensing portion is equal to the magnetic flux of the permanent magnet film in the same direction.
Set the direction of. That is, when the magnetization direction of the permanent magnet film and theta, have set theta to (B h · t h) cosθ ≒ (B m · t m) cos45 ° ...... (3). (Third Embodiment) FIG. 4 is a configuration diagram showing a third embodiment of the present invention. Referring to FIG. 4, the third embodiment relates to a specific material configuration of the MR element. The MR film 11 is made of a NiFe film, and B m ≒ 850.
0G, t m ≒ 20 nm. Further, a Ta film having a thickness of 10 nm is used as the nonmagnetic film 12. Further, the SAL film 13
Is composed of an amorphous CoZrMo film and has a saturation magnetic flux density B s ≒
6000 G, thickness t s ≒ 20 nm. In this case, conditional expression (2) is satisfied.
【0018】次に、永久磁石膜2は、厚さ10nmのC
r膜を下地として、飽和磁束密度Bh ≒8000GのC
oCrPt膜を、膜厚th ≒20nmでスパッタ成膜法
により作製している。これは条件式(1) を満足してい
る。そして、さらに条件式(3)を満足するように角度θ
を設定する。Next, the permanent magnet film 2 has a thickness of 10 nm.
With the r film as the base, the saturation magnetic flux density B h C
An oCrPt film is formed with a thickness t h ≒ 20 nm by a sputtering film forming method. This satisfies conditional expression (1). Then, the angle θ is set so as to further satisfy the conditional expression (3).
Set.
【0019】そうすると、永久磁石膜2は(Bh ・
th )≒160000G・nmであり、また、MR膜1
1は(Bm ・tm )cos45°≒120000G・n
mであるので、θ≒41゜に設定すると、条件式(3) を
満足する。 (実施の形態4)図9を参照して本発明の実施の形態4
について説明する。本実施の形態4は、永久磁石膜を感
磁部のMR膜の磁区安定化のバイアス膜とした、MR効
果型磁気ヘッドの例である。本例は、実施の形態3で示
した膜構造の感磁部1と永久磁石膜2とから成るMR素
子を、厚さ2μmのNiFe合金膜の下シールド31
と、厚さ3μmのNiFe合金膜の上シールド32との
間に絶縁層を介して設けたシールド型MRヘッドであ
る。Then, the permanent magnet film 2 becomes (B h ·
t h ) ≒ 160000 G · nm and MR film 1
1 is (B m · t m ) cos 45 ° @ 120,000 G · n
m, the condition (3) is satisfied when θ is set to {41}. (Embodiment 4) Embodiment 4 of the present invention with reference to FIG.
Will be described. The fourth embodiment is an example of an MR effect type magnetic head in which a permanent magnet film is used as a bias film for stabilizing the magnetic domain of the MR film of the magnetosensitive portion. In this example, the MR element including the magneto-sensitive part 1 and the permanent magnet film 2 having the film structure shown in the third embodiment is replaced with a NiFe alloy film lower shield 31 having a thickness of 2 μm.
And a shield type MR head provided with an insulating layer between the upper shield 32 and a 3 μm thick NiFe alloy film.
【0020】このような構造にすることにより、分解能
の高い再生用のMRヘッドを得る。なお、本例では、記
録素子は省略されているが、記録素子と結合した複合型
MRヘッドでも、本発明は容易に実施できることは明白
である。 (実施の形態5) 図10及び図11を参照して本発明の実施の形態5につ
いて説明する。本実施の形態5は、永久磁石膜の着磁に
より磁化方向を決定する製造方法に関するものである。
まず、図10に示すように、本発明にかかわるMRヘッ
ドに、センス電流印加手段IとMR素子の抵抗変化を検
出する電圧検知手段Vを接続する。さらに、磁界−抵抗
応答曲線を得るための抵抗−磁界測定手段、外部交流磁
界Hを印加する交流磁界印加手段、永久磁石膜の磁化方
向を決定する磁化方向回転手段、永久磁石膜に着磁用直
流磁界Hh を印加する着磁手段を備える。By adopting such a structure, an MR head for reproduction with high resolution is obtained. Although the recording element is omitted in this example, it is apparent that the present invention can be easily implemented even with a composite MR head combined with the recording element. Embodiment 5 Embodiment 5 of the present invention will be described with reference to FIGS. The fifth embodiment relates to a manufacturing method for determining a magnetization direction by magnetizing a permanent magnet film.
First, as shown in FIG. 10, a sense current applying means I and a voltage detecting means V for detecting a change in resistance of an MR element are connected to an MR head according to the present invention. Furthermore, resistance-magnetic field measuring means for obtaining a magnetic field-resistance response curve, AC magnetic field applying means for applying an external AC magnetic field H, magnetization direction rotating means for determining the magnetization direction of the permanent magnet film, A magnetizing means for applying a DC magnetic field Hh is provided.
【0021】図11は、永久磁石膜に対する着磁のプロ
セスを説明する構成図である。図11を参照すると、本
プロセスにかかわる着磁手段は、MR素子(感磁部1,
永久磁石膜2)に交流磁界Hを印加する交流磁界印加手
段41と、抵抗−磁界応答を測定する抵抗−磁界測定手
段42と、その応答からバルクハウゼンノイズの有無を
判定するバルクハウゼン判定回路43と、この判定結果
により着磁磁界の方向を変更する磁界方向回転手段44
と、永久磁石膜2に着磁磁界Hh を印可する着磁手段4
5とから成る。そして、抵抗−磁界測定手段42から求
めた抵抗−磁界応答曲線により、バルクハウゼンノイズ
が生じなくなるように、着磁方向を変更することによ
り、永久磁石膜2の磁化方向をθを最適化する。FIG. 11 is a configuration diagram illustrating the process of magnetizing the permanent magnet film. Referring to FIG. 11, the magnetizing means related to the present process is an MR element (magnetic sensing unit 1,
AC magnetic field applying means 41 for applying an AC magnetic field H to the permanent magnet film 2), resistance-magnetic field measuring means 42 for measuring a resistance-magnetic field response, and a Barkhausen determination circuit 43 for determining the presence or absence of Barkhausen noise from the response Magnetic field direction rotating means 44 for changing the direction of the magnetizing magnetic field based on the result of the determination.
When magnetizing means 4 for applying the magnetizing magnetic field H h permanent magnet film 2
5 Then, the magnetization direction of the permanent magnet film 2 is optimized by changing the magnetization direction according to the resistance-magnetic field response curve obtained from the resistance-magnetic field measuring means 42 so that Barkhausen noise does not occur.
【0022】[0022]
【発明の効果】以上説明したように本発明を用いること
により、磁界検出感度の低下を招くことなく、歩留まり
が高くかつバルクハウゼンノイズの発生を抑制したMR
素子、MRヘッド及びその製造方法を提供できる。As described above, by using the present invention, an MR having a high yield and suppressing the generation of Barkhausen noise without lowering the magnetic field detection sensitivity.
An element, an MR head, and a method of manufacturing the same can be provided.
【図1】本発明の第1の実施の形態を示す構成図であ
る。FIG. 1 is a configuration diagram showing a first embodiment of the present invention.
【図2】本発明の第2の実施の形態を示す構成図であ
る。FIG. 2 is a configuration diagram showing a second embodiment of the present invention.
【図3】本発明の第2の実施の形態を示す構成図であ
る。FIG. 3 is a configuration diagram showing a second embodiment of the present invention.
【図4】本発明の第3の実施の形態を示す構成図であ
る。FIG. 4 is a configuration diagram showing a third embodiment of the present invention.
【図5】従来の磁気抵抗効果素子の一例を示す図であ
る。FIG. 5 is a diagram showing an example of a conventional magnetoresistance effect element.
【図6】従来の磁気抵抗効果素子の一例を示す図であ
る。FIG. 6 is a diagram showing an example of a conventional magnetoresistance effect element.
【図7】ある磁界で急激に抵抗変化を生じる抵抗−磁界
応答曲線を示す図である。FIG. 7 is a diagram showing a resistance-magnetic field response curve that causes a rapid change in resistance in a certain magnetic field.
【図8】良好な抵抗−磁界応答曲線を示す図である。FIG. 8 is a diagram showing a good resistance-magnetic field response curve.
【図9】本発明の第4の実施の形態を示す斜視図であ
る。FIG. 9 is a perspective view showing a fourth embodiment of the present invention.
【図10】本発明の第5の実施の形態を示す構成図であ
る。FIG. 10 is a configuration diagram showing a fifth embodiment of the present invention.
【図11】本発明の第5の実施の形態を実現する構成図
である。FIG. 11 is a configuration diagram for realizing a fifth embodiment of the present invention.
1 感磁部 2 永久磁石膜 11 MR膜 12 非磁性膜 13 SAL膜(隣接軟磁性膜) 15 MR膜磁化方向 25 永久磁石膜磁化方向 31 下シールド 32 上シールド 41 交流磁界印加手段 42 抵抗−磁界測定手段 43 バルクハウゼンノイズ判定手段 44 磁界方向回転手段 45 着磁手段 H 交流磁界 I センス電流印加手段(電流源) J センス電流方向 V 感磁部抵抗測定手段(電圧計測部) Hh 着磁磁界 th 永久磁石膜膜厚 tm MR膜膜厚 ts SAL膜膜厚DESCRIPTION OF SYMBOLS 1 Magnetic sensing part 2 Permanent magnet film 11 MR film 12 Non-magnetic film 13 SAL film (adjacent soft magnetic film) 15 MR film magnetization direction 25 Permanent magnet film magnetization direction 31 Lower shield 32 Upper shield 41 AC magnetic field applying means 42 Resistance-magnetic field Measuring means 43 Barkhausen noise determining means 44 Magnetic field direction rotating means 45 Magnetizing means H AC magnetic field I Sense current applying means (current source) J Sense current direction V Sensitive part resistance measuring means (Voltage measuring part) H h Magnetizing magnetic field t h permanent magnet MakumakuAtsu t m MR MakumakuAtsu t s SAL MakumakuAtsu
Claims (7)
感磁部と、この感磁部に印加されるセンス電流と、前記
感磁部の両側に設けた永久磁石膜で形成される磁区安定
パタンとを有する磁気抵抗効果素子において、 前記磁区安定パタンの磁化方向と前記センス電流の印加
方向とが実質的に非平行であることを特徴とする磁気抵
抗効果素子。1. A magnetic sensing part formed of a magnetic film exhibiting a magnetoresistive effect, a sense current applied to the magnetic sensing part, and a magnetic domain formed by a permanent magnet film provided on both sides of the magnetic sensing part. A magnetoresistive element having a stable pattern, wherein the direction of magnetization of the magnetic domain stable pattern and the direction of application of the sense current are substantially non-parallel.
膜厚を各々Bm ,tm 、前記磁性膜の磁化方向と前記セ
ンス電流の印加方向とのなす角をα、前記センス電流の
印加方向と前記永久磁石膜の磁化方向とのなす角をθ、
前記永久磁石膜の飽和磁束密度及び膜厚を各々Bh ,t
h とするとき、 (Bm ・tm )cosα≧(Bh ・th )cosθ を満たすように、前記θを定めることを特徴とする特許
請求の範囲第1項記載の磁気抵抗効果素子。2. The saturation magnetic flux density and the thickness of the magnetic film of the magnetic sensing portion are B m and t m , respectively, the angle between the magnetization direction of the magnetic film and the direction of application of the sense current is α, and the sense current is α. Is the angle between the direction of application and the magnetization direction of the permanent magnet film, θ,
Saturation magnetic flux density and each thickness B h of the permanent magnet film, t
2. The magnetoresistive element according to claim 1, wherein, when h is set, the angle θ is determined so as to satisfy (B m · t m ) cos α ≧ (B h · th h ) cos θ.
膜厚を各々Bm ,tm 、前記磁性膜の磁化方向と前記セ
ンス電流の印加方向とのなす角αがほぼ45°、前記永
久磁石膜の飽和磁束密度及び膜厚を各々Bh ,th とす
るとき、 (Bm ・tm )cosα<(Bh ・th ) であることを特徴とする特許請求の範囲第1項記載の磁
気抵抗効果素子。3. The saturation magnetic flux density and the film thickness of the magnetic film of the magnetic sensing portion are B m and t m , respectively, and the angle α between the magnetization direction of the magnetic film and the sense current application direction is approximately 45 °, saturation magnetic flux density and each thickness B h of the permanent magnet film, when a t h, the claims, which is a (B m · t m) cosα <(B h · t h) 2. The magnetoresistance effect element according to claim 1.
の磁気抵抗効果素子を膜厚方向に両側から磁気シールド
とを備えることを特徴とする磁気抵抗効果型磁気ヘッ
ド。4. A magnetoresistance effect type magnetic head comprising: the magnetoresistance effect element according to claim 1; and a magnetic shield from both sides of the magnetoresistance effect element in a film thickness direction.
の磁気抵抗効果素子を膜厚方向に両側から磁気シールド
とを備えることを特徴とする磁気抵抗効果型磁気ヘッ
ド。5. A magnetoresistive effect type magnetic head comprising: the magnetoresistive effect element according to claim 2; and a magnetic shield from both sides of the magnetoresistive effect element in a film thickness direction.
の磁気抵抗効果素子を膜厚方向に両側から磁気シールド
とを備えることを特徴とする磁気抵抗効果型磁気ヘッ
ド。6. A magnetoresistive effect type magnetic head comprising: the magnetoresistive element according to claim 3; and a magnetic shield comprising the magnetoresistive element from both sides in a film thickness direction.
気抵抗効果型磁気ヘッドの製造方法であって、 前記磁気抵抗効果素子に交流磁界を印加しながら前記磁
気抵抗効果素子の抵抗−磁界応答を測定し、かつこの測
定結果に基づいて前記磁気抵抗効果素子の永久磁石膜の
着磁方向を任意に変更し、前記永久磁石膜の磁化方向を
最適化するようにしたことを特徴とする磁気抵抗効果型
磁気ヘッドの製造方法。7. The method of manufacturing a magnetoresistive effect type magnetic head according to claim 4, wherein a resistance of the magnetoresistive effect element is reduced by applying an AC magnetic field to the magnetoresistive effect element. The magnetic field response is measured, and the magnetization direction of the permanent magnet film of the magnetoresistive effect element is arbitrarily changed based on the measurement result to optimize the magnetization direction of the permanent magnet film. Of manufacturing a magnetoresistive magnetic head.
Priority Applications (1)
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---|---|---|---|
JP7241572A JP2798016B2 (en) | 1995-09-20 | 1995-09-20 | Magnetoresistive element, magnetoresistive head and method of manufacturing the same |
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JP7241572A JP2798016B2 (en) | 1995-09-20 | 1995-09-20 | Magnetoresistive element, magnetoresistive head and method of manufacturing the same |
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JP2798016B2 true JP2798016B2 (en) | 1998-09-17 |
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