JPH02130712A - Magneto-resistance effect element - Google Patents

Magneto-resistance effect element

Info

Publication number
JPH02130712A
JPH02130712A JP63283594A JP28359488A JPH02130712A JP H02130712 A JPH02130712 A JP H02130712A JP 63283594 A JP63283594 A JP 63283594A JP 28359488 A JP28359488 A JP 28359488A JP H02130712 A JPH02130712 A JP H02130712A
Authority
JP
Japan
Prior art keywords
magnetoresistive
film
magnetic
magneto
layer
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
JP63283594A
Other languages
Japanese (ja)
Inventor
Hideo Tanabe
英男 田辺
Masahiro Kitada
北田 正弘
Noboru Shimizu
昇 清水
Hitoshi Nakamura
斉 中村
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.)
Hitachi Ltd
Original Assignee
Hitachi Ltd
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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP63283594A priority Critical patent/JPH02130712A/en
Publication of JPH02130712A publication Critical patent/JPH02130712A/en
Pending legal-status Critical Current

Links

Classifications

    • 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
    • G11B5/127Structure or manufacture of heads, e.g. inductive
    • G11B5/33Structure or manufacture of flux-sensitive heads, i.e. for reproduction only; Combination of such heads with means for recording or erasing only
    • G11B5/39Structure or manufacture of flux-sensitive heads, i.e. for reproduction only; Combination of such heads with means for recording or erasing only using magneto-resistive devices or effects
    • G11B5/3903Structure or manufacture of flux-sensitive heads, i.e. for reproduction only; Combination of such heads with means for recording or erasing only using magneto-resistive devices or effects using magnetic thin film layers or their effects, the films being part of integrated structures
    • G11B5/398Specially shaped layers
    • 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
    • G11B5/127Structure or manufacture of heads, e.g. inductive
    • G11B5/33Structure or manufacture of flux-sensitive heads, i.e. for reproduction only; Combination of such heads with means for recording or erasing only
    • G11B5/39Structure or manufacture of flux-sensitive heads, i.e. for reproduction only; Combination of such heads with means for recording or erasing only using magneto-resistive devices or effects
    • G11B5/3903Structure or manufacture of flux-sensitive heads, i.e. for reproduction only; Combination of such heads with means for recording or erasing only using magneto-resistive devices or effects using magnetic thin film layers or their effects, the films being part of integrated structures

Abstract

PURPOSE:To improve the output of a magneto-resistance effect element by not providing a thin film of a soft magnetic substance for guiding magnetic fluxes of signals, but only protruding a magnetism sensible section corresponding to the signal recording track width on a magnetic recording medium at the central part of a magneto- resistance effect film from the surface of the element facing the medium. CONSTITUTION:After an insulating layer 2 of an Al2O3 film, etc., is formed to a thickness of 0.1-0.4mum on a base plate 1 which is made of a magnetic substance of ferrite, etc., and also works as a lower magnetic shield, a film 3 of a good conductor of Al, Cu, etc., for impressing a bias magnetic field upon a magneto-resistance effect film 5 is formed and patterned to a thickness of 0.05-0.2mum on the layer 2. Then, after forming an insulating layer 4 similar to the layer 2 on the film 3, the magneto- resistance effect film 5 of a thin film of an Ni-Fe alloy, etc., is formed and patterned to a thickness of 10-100nm on the insulating layer 4. Thereafter, a magnetic substance belt 5' for guiding magnetic fluxes having a width almost equal to the width of a magnetism sensible section 6 is provided on the side opposite to the medium facing surface 8 of this magneto-resistance effect element by protruding the magnetism sensible section 6 of the effect film 5 from the medium facing surface 8 and retreating the other section from the surface 8.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、再生専用の磁気抵抗効果型ヘッドに使用する
磁気抵抗効果素子に係り、特に狭トラツク幅の磁化再生
に好適な磁気抵抗効果素子に関する。
[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a magnetoresistive element used in a read-only magnetoresistive head, and particularly to a magnetoresistive element suitable for magnetization reproduction with a narrow track width. Regarding.

〔従来の技術〕[Conventional technology]

従来の磁気抵抗効果素子は、特開昭57−181425
号および特開昭59−24427号に記載のように、媒
体対向面から離して設けられた磁気抵抗効果素子の感磁
部に磁気記録媒体からの信号磁束を導くための磁束導入
用軟磁性体薄膜を別に設けていた。
The conventional magnetoresistive element is disclosed in Japanese Patent Application Laid-Open No. 57-181425.
and JP-A No. 59-24427, a soft magnetic material for introducing magnetic flux for guiding signal magnetic flux from a magnetic recording medium to a magnetic sensing part of a magnetoresistive element provided apart from a medium facing surface. A thin film was provided separately.

また、特開昭50−65211号に記載のように、磁気
抵抗効果素子の出力を増加しノイズを低減するために、
該磁気抵抗効果素子に使用する磁気抵抗効果膜を絶縁層
を介した2層とし、各磁気抵抗効果膜の出力の差あるい
は和をとって増幅していた。
In addition, as described in Japanese Patent Application Laid-Open No. 50-65211, in order to increase the output of the magnetoresistive element and reduce noise,
The magnetoresistive film used in the magnetoresistive element has two layers with an insulating layer interposed therebetween, and the difference or sum of the outputs of each magnetoresistive film is amplified.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

上記特開昭57−181425号記載の従来技術では、
信号磁束導入用軟磁性体薄膜と磁気抵抗効果膜の感磁部
との間に絶縁層を設ける。このために上記両者間の磁気
抵抗が増加し、実質的に該感磁部に導入される信号磁束
の量が低下する。従って、当該磁気抵抗効果素子の信号
再生効率が低下するという問題があった。
In the prior art described in JP-A No. 57-181425,
An insulating layer is provided between the soft magnetic thin film for introducing signal magnetic flux and the magnetically sensitive portion of the magnetoresistive film. For this reason, the magnetic resistance between the two increases, and the amount of signal magnetic flux introduced into the magnetically sensitive portion substantially decreases. Therefore, there is a problem in that the signal reproduction efficiency of the magnetoresistive element is reduced.

また、上記特開昭50−65211号記載の従来技術で
は、2層に形成された各々の磁気抵抗効果膜に信号磁束
が吸われるのに時間的な差があるため、必然的に各磁気
抵抗効果膜の出力波形間に位相差が発生する。このため
各磁気抵抗効果膜の出力の差あるいは和を増幅して得ら
れる当該磁気抵抗効果素子の出力波形が大きく歪む、と
いう問題があつた。
Furthermore, in the prior art described in JP-A-50-65211, since there is a time difference in the absorption of signal magnetic flux by each magnetoresistive film formed in two layers, it is inevitable that each magnetoresistive A phase difference occurs between the output waveforms of the effect film. For this reason, there has been a problem in that the output waveform of the magnetoresistive element obtained by amplifying the difference or sum of the outputs of the respective magnetoresistive films is greatly distorted.

本発明の目的は、上記問題をなくし狭トラツク幅の磁化
再生に好適な磁気抵抗効果素子を提供することにある。
SUMMARY OF THE INVENTION An object of the present invention is to provide a magnetoresistive element which eliminates the above-mentioned problems and is suitable for magnetization reproduction with a narrow track width.

〔11!!題を解決するための手段〕 本発明においては上記目的を達成するために信号磁束導
入用の軟磁性体薄膜を設けず、該磁気抵抗効果膜の中心
部で磁気記録媒体上に記録された信号の記録トラック幅
に対応する感磁部分だけ媒体対向面に突出させ、その他
の残りの磁気抵抗効果膜上に検出電流導入用のリード線
を設けた構造とする。
[11! ! Means for Solving the Problem] In order to achieve the above object, the present invention does not provide a soft magnetic thin film for introducing signal magnetic flux, and the signal recorded on the magnetic recording medium at the center of the magnetoresistive film is Only the magnetically sensitive portion corresponding to the recording track width of is made to protrude from the medium facing surface, and a lead wire for introducing a detection current is provided on the remaining magnetoresistive film.

さらに、上記磁気抵抗効果膜を絶縁層を介した2層とし
て下層の磁気抵抗効果膜にも同様の検出電流導入用のリ
ード線を設け、ただし媒体対向面をその近傍の上記突出
部においては絶縁層を除去して上層および下層の磁気抵
抗効果膜を互いに接触させることにより、より好ましい
結果が得られる。
Further, the magnetoresistive film is formed into two layers with an insulating layer interposed therebetween, and a similar lead wire for introducing a detection current is provided in the lower magnetoresistive film, however, the medium facing surface is insulated at the protrusion near it. A more favorable result can be obtained by removing the layer and bringing the upper and lower magnetoresistive films into contact with each other.

〔作用〕[Effect]

本発明では、上述したように信号磁束導入用の軟磁性体
薄膜を設けずに該磁気抵抗効果膜の感磁部分だけ突出さ
せることにより、記録媒体からの信号磁束をこの突出部
から吸い込んで直接磁気抵抗効果膜の感磁部に導くこと
が可能となる。さらにこのように感磁部内体を突出させ
るユとア感磁部の反磁界を低下することが可能となる。
In the present invention, as described above, by protruding only the magnetically sensitive part of the magnetoresistive film without providing a soft magnetic thin film for introducing signal magnetic flux, the signal magnetic flux from the recording medium is sucked in from this protruding part and directly transmitted. It becomes possible to guide the magnetic field to the magnetically sensitive part of the magnetoresistive film. Furthermore, by protruding the internal body of the magnetically sensitive part in this way, it becomes possible to reduce the demagnetizing field of the magnetically sensitive part.

それによって、上記信号磁束量を減少させることなく感
磁部に導くことができる。
Thereby, the signal magnetic flux can be guided to the magnetic sensing part without decreasing the amount of signal magnetic flux.

また、2層とした磁気抵抗効果膜において、上記突出部
の媒体対向面とその近傍で磁気抵抗効果膜間の絶縁層を
除去して上下の磁気抵抗効果膜を互いに接触させること
により、信号磁束を同時に上下の磁気抵抗効果膜の感磁
部に導くことが可能となる。それによって、上下の磁気
抵抗効果膜の出力の差あるいは和をとって増幅した場合
においても、得られる出力波形に歪みを生ずることがな
くなる。
In addition, in a two-layer magnetoresistive film, by removing the insulating layer between the magnetoresistive films at the medium facing surface of the protrusion and its vicinity, and bringing the upper and lower magnetoresistive films into contact with each other, the signal magnetic flux can be guided to the magnetically sensitive parts of the upper and lower magnetoresistive films at the same time. Thereby, even when the difference or the sum of the outputs of the upper and lower magnetoresistive films is amplified, no distortion occurs in the resulting output waveform.

【実施例〕【Example〕

以下、本発明を実施例により詳しく説明する。 Hereinafter, the present invention will be explained in detail with reference to Examples.

実施例1 第1図(a)は本発明の一実施例による磁気抵抗効果素
子の正面図、同図(b)は同図(a)のA−A’断面図
である。
Embodiment 1 FIG. 1(a) is a front view of a magnetoresistive element according to an embodiment of the present invention, and FIG. 1(b) is a sectional view taken along line AA' in FIG. 1(a).

本実施例では、フェライトなどの磁性体からなる下部磁
気シールドを兼ねた基板1(あるいはセラミックスなど
の非磁性体上にAΩ208膜などの絶縁層を介して下部
磁気シールド用の軟磁性体薄膜を積層した基板でもよい
)を用いた。この基板lの上にAQxOsmや5iOz
膜などからなる絶縁層2をスパッタ法等により0.1〜
0.4μm積層する。その上に磁気抵抗効果膜5にバイ
アス磁界を印加するためのAffあるいはCuなどの良
導体からなる導電体膜3を0,05〜0.2μmの厚さ
に蒸着法あるいはスパッタ法により積層する。
In this example, a soft magnetic thin film for the lower magnetic shield is laminated on a substrate 1 made of a magnetic material such as ferrite that also serves as a lower magnetic shield (or on a non-magnetic material such as ceramics through an insulating layer such as an AΩ208 film). (It may also be possible to use a On this substrate l, AQxOsm and 5iOz
The insulating layer 2 made of a film or the like is formed by sputtering or the like to a thickness of 0.1 to
Laminate 0.4 μm thick. Thereon, a conductor film 3 made of a good conductor such as Aff or Cu for applying a bias magnetic field to the magnetoresistive film 5 is laminated to a thickness of 0.05 to 0.2 μm by vapor deposition or sputtering.

そしてホトリソグラフィの手法とドライエツチング法と
により所定の形状にパターニングした。
Then, it was patterned into a predetermined shape using photolithography and dry etching.

さらにこの上に、上述した絶縁N2と同様の材質からな
る厚さ0.1〜0.2μmの絶縁層4を形成する。そし
てこの絶縁層4上にN1−Fa合金薄膜やN i −G
 o合金薄膜などの磁気抵抗効果ヲ有する磁気抵抗効果
膜5を、蒸着法あるいはスパッタ法等により10〜11
00n厚さに積層し、ホトリソグラフィの手法とドライ
エツチング法とにより所定の形状にパターニングした。
Furthermore, an insulating layer 4 having a thickness of 0.1 to 0.2 μm and made of the same material as the above-mentioned insulating layer N2 is formed thereon. Then, on this insulating layer 4, an N1-Fa alloy thin film or a Ni-G
o A magnetoresistive film 5 having a magnetoresistive effect, such as an alloy thin film, is formed by a vapor deposition method, a sputtering method, etc.
The layers were laminated to a thickness of 00 nm, and patterned into a predetermined shape by photolithography and dry etching.

この形状の特徴は、上記磁気抵抗効果膜上の感磁部6だ
けを磁気記録媒体7に対向する媒体対向面8に突出させ
、その他の部分は媒体対向面8から引込め、さらに感磁
部6の媒体対向面8と反対側に、0.5〜1μmの間隔
をおいて感磁部6の幅とほぼ等しい磁束ガイド用の磁性
体の帯5′を設けたことである。
The feature of this shape is that only the magnetically sensitive portion 6 on the magnetoresistive film protrudes to the medium facing surface 8 that faces the magnetic recording medium 7, and the other portions are retracted from the medium facing surface 8. On the side opposite to the medium facing surface 8 of 6, a band 5' of magnetic material for guiding magnetic flux is provided at an interval of 0.5 to 1 .mu.m, and the width is approximately equal to the width of the magnetically sensitive portion 6.

突出させる感磁部6の幅は磁気記録媒体7上のトラック
幅に等しく、突出させる長さは、磁気抵抗効果素子を磁
気記録媒体上で稼動させた時の最大摩耗量以上であれば
よい。ただし、該突出部の長さは本発明を使用する装置
によって適正化することが望ましい。例えば磁気ディス
ク装置などの摩耗量が少ない装置に使用する場合には、
突出部の長さは1〜10μmの範囲が望ましいが、この
場合突出部の幅も10μm以下が望ましい。また磁気テ
ープ装置など摩耗量の多い装置に使用する場合には、突
出部の長さは摩耗量に合わせて摩耗量+2〜5μmにす
るのが望ましい。
The width of the protruding magnetically sensitive portion 6 is equal to the track width on the magnetic recording medium 7, and the protruding length may be equal to or greater than the maximum wear amount when the magnetoresistive element is operated on the magnetic recording medium. However, it is desirable that the length of the protrusion be optimized by the device using the present invention. For example, when used in devices with low wear such as magnetic disk drives,
The length of the protrusion is preferably in the range of 1 to 10 μm, but in this case, the width of the protrusion is also preferably 10 μm or less. In addition, when used in a device with a large amount of wear such as a magnetic tape device, it is desirable that the length of the protrusion is set to the amount of wear plus 2 to 5 μm in accordance with the amount of wear.

なお、上記磁気抵抗効果膜5の容易磁化方向は、磁気抵
抗効果膜5の長手方向と平行にした。
Note that the easy magnetization direction of the magnetoresistive film 5 was parallel to the longitudinal direction of the magnetoresistive film 5.

そして上記磁気抵抗効果膜5の感磁部6以外の膜上に信
号検出電流導入用のAQあるいはCuなどからなる電流
導入線9を形成し、さらにAl2011膜やS i O
2膜からなる絶縁層10を0.1〜0.8μmの厚さで
積層し、最後に上部シールド用の軟磁性体薄膜11を積
層して(あるいはフェライトなどの軟磁性体を接着剤等
で接合してもよい)磁気抵抗効果素子12の作製を終了
した。
Then, a current introducing line 9 made of AQ or Cu for introducing a signal detection current is formed on the film other than the magnetically sensitive part 6 of the magnetoresistive film 5, and is further made of an Al2011 film or SiO.
An insulating layer 10 consisting of two films is laminated with a thickness of 0.1 to 0.8 μm, and finally a soft magnetic thin film 11 for the upper shield is laminated (or a soft magnetic material such as ferrite is laminated with an adhesive or the like). The production of the magnetoresistive element 12 (which may be bonded) has been completed.

本実施例による磁気抵抗効果素子12では、磁気記録媒
体から漏れ出る信号磁束13を媒体対向面8に突出した
磁気抵抗効果膜から吸い込んで直接感磁部6に導き、さ
らに、感磁部6を通って磁束ガイド用の磁性体の帯5′
まで導く。この結果この感磁部6において、感磁部に導
かれた信号磁束、ユよ、感磁部6の抵抗が磁気抵抗効果
テ変化スるのを利用して、検出電流導入線9から該抵抗
変化に対応した電圧変化を検出する。これによツア磁気
記録媒体7上に記録された信号を読み取る工とができる
。この際、上記磁気抵抗効果膜5の感磁部6に、該感磁
部内の磁化の向きが検出電流の方向に対して略45°の
角度をなすように導電体膜3に適当な電流を与えてバイ
アス磁界を印加しておく必要がある。
In the magnetoresistive element 12 according to this embodiment, the signal magnetic flux 13 leaking from the magnetic recording medium is sucked in through the magnetoresistive film protruding from the medium facing surface 8 and guided directly to the magnetically sensitive part 6. A magnetic strip 5' for guiding the magnetic flux through the
lead to. As a result, in this magnetic sensing part 6, the signal magnetic flux guided to the magnetic sensing part, the resistance of the magnetic sensing part 6 changes due to the magnetoresistive effect, and the detection current introduction line 9 is connected to the resistance. Detects voltage changes corresponding to changes. This makes it possible to read the signals recorded on the tour magnetic recording medium 7. At this time, an appropriate current is applied to the conductor film 3 in the magnetically sensitive part 6 of the magnetoresistive film 5 so that the direction of magnetization in the magnetically sensitive part forms an angle of approximately 45° with respect to the direction of the detection current. It is necessary to apply a bias magnetic field.

本実施例によれば、上述したように媒体対向面8に突出
させた磁気抵抗効果膜5から直接信号磁束13を感磁部
6に導くことができるので、媒体対向面より吸い込んだ
信号磁束量を漏洩のために減少させることなく感磁部6
に導くことが可能となり、当該磁気抵抗効果素子12の
出力を従来の磁気抵抗効果素子よりも高める効果がある
According to this embodiment, as described above, the signal magnetic flux 13 can be directly guided from the magnetoresistive film 5 protruding from the medium facing surface 8 to the magnetic sensing part 6, so the amount of signal magnetic flux absorbed from the medium facing surface magnetically sensitive part 6 without reducing due to leakage.
This has the effect of increasing the output of the magnetoresistive element 12 more than that of a conventional magnetoresistive element.

実施例2 第2図(a)は本発明の他の実施例による磁気抵抗効果
素子の正面図、同図(b)は同図(a)のB−B’断面
図、同図(Q)は同図(a)のC−C′断面図である。
Embodiment 2 FIG. 2(a) is a front view of a magnetoresistive element according to another embodiment of the present invention, FIG. 2(b) is a sectional view taken along line BB' in FIG. 2(a), and FIG. is a sectional view taken along line CC' in FIG.

本実施例では、実施例1の場合と同様の基板1上に積層
した絶縁層2上に、フォトリングラフィ法およびドライ
エツチング法により検出電流導入線9を設けるための溝
14を形成し、この溝14の中にAQあるいはCuなど
からなる電流導入線91を設けた。この後に第1層目の
N i −F e合金あるいはN i −Co合金など
からなる磁気抵抗効果膜51を蒸着法あるいはスパッタ
法等により10〜1100nの厚さに積層し、実施例1
の場合と同様の方法で同様な形状にパターニングした。
In this example, a groove 14 for providing a detection current lead-in line 9 is formed on an insulating layer 2 laminated on a substrate 1 similar to that in Example 1 by photolithography and dry etching. A current introduction line 91 made of AQ, Cu, or the like is provided in the groove 14. Thereafter, a first layer of magnetoresistive film 51 made of Ni-Fe alloy or Ni-Co alloy is laminated to a thickness of 10 to 1100 nm by vapor deposition or sputtering, thereby forming the structure of Example 1.
It was patterned into a similar shape using the same method as in the case of .

この時、磁気抵抗効果膜51と電流導入!91とを接触
させ互いに導通するようにした。次にこの上に、上記絶
縁層2と同質の絶縁層15を0.05〜0.4μm厚で
積層し、第2層目の磁気抵抗効果膜52を第1層目の磁
気抵抗効果膜51と同厚。
At this time, current is introduced into the magnetoresistive film 51! 91 so that they are electrically connected to each other. Next, an insulating layer 15 of the same quality as the insulating layer 2 is laminated thereon to a thickness of 0.05 to 0.4 μm, and the second layer magnetoresistive film 52 is stacked on top of the first layer magnetoresistive film 51. Same thickness.

同形状に、同様に作製方法で形成した。It was formed into the same shape and by the same manufacturing method.

ここで重要なことは、上記第2層目の磁気抵抗効果膜5
2を積層する前に媒体対向面8とその近傍の絶縁層15
中にスルホール16を開けて、第2層目の磁気抵抗効果
膜52の突出部と第1層目の磁気抵抗効果膜51の突出
部とを媒体対向面8とその近傍で接触させたことである
。該突出部の長さおよび幅は実施例1の場合と同様に1
本実施例を使用する装置によって適正化することが望ま
しく、その値は実施例1の場合と同様である。なお、第
2層目の磁気抵抗効果膜52の容易磁化方向は第1層目
の磁気抵抗効果膜51と同様にパターンの長軸方向と平
行とした。そして、第2層目の磁気抵抗効果[52上に
検出電流導入線92を設けたが、やはりこの際、磁気抵
抗効果膜52のいずれか一方の端部側、本実施例では右
端部側の絶縁層15中にスルーホール17を開けて、当
該検出電流導入線92と第1層目の磁気抵抗効果膜51
下の右端部側の検出電流導入線91とを短絡させるよう
にした。
What is important here is that the second layer magnetoresistive film 5
2, before laminating the medium facing surface 8 and the insulating layer 15 in its vicinity.
By opening a through hole 16 inside, the protrusion of the second layer magnetoresistive film 52 and the protrusion of the first layer magnetoresistive film 51 are brought into contact with the medium facing surface 8 and its vicinity. be. The length and width of the protrusion are 1 as in Example 1.
It is desirable to optimize the value depending on the device using this embodiment, and the value is the same as in the first embodiment. Note that the easy magnetization direction of the second layer magnetoresistive film 52 was parallel to the long axis direction of the pattern similarly to the first layer magnetoresistive film 51. Then, the detection current introduction line 92 was provided on the second layer magnetoresistive film 52, but at this time, the detection current lead-in line 92 was provided on either one end side of the magnetoresistive film 52, in this example, on the right end side. A through hole 17 is opened in the insulating layer 15, and the detection current introducing line 92 and the first layer magnetoresistive film 51 are connected to each other.
The detection current lead-in line 91 on the lower right end side is short-circuited.

そして最後に、実施例1の場合と同様に絶縁層10を積
層し、上部磁気シールド層11を形成して磁気抵抗効果
素子18の作製を終了した。なお、本実施例では実施例
1の場合のようなバイアス磁界印加用の導電体膜3を設
けてないが、これは磁気抵抗効果膜を2層としたことに
より、各磁気抵抗効果膜に検出電流を流せば相互にバイ
アスする効果が働くためである。
Finally, in the same manner as in Example 1, the insulating layer 10 was laminated and the upper magnetic shield layer 11 was formed to complete the production of the magnetoresistive element 18. In this example, unlike the case of Example 1, the conductive film 3 for applying a bias magnetic field is not provided, but this is because the magnetoresistive film has two layers, so that each magnetoresistive film can detect the This is because when current flows, there is a mutual biasing effect.

以上述べたような本実施例による磁気抵抗効果素子18
では、媒体対向面8に突出した磁気抵抗効果膜51.5
2から同時に磁気記録媒体7から漏れ出る信号磁束13
を吸い込み、直接上層、下層の磁気抵抗効果膜の感磁部
61,62に導き、さらに感磁部61,62を通って磁
束ガイド用の磁性体の帯51’ 、52’ まで導く。
Magnetoresistive element 18 according to this embodiment as described above
Now, the magnetoresistive film 51.5 protruding from the medium facing surface 8
Signal magnetic flux 13 simultaneously leaking from magnetic recording medium 7 from 2
is sucked in and guided directly to the magnetically sensitive parts 61 and 62 of the upper and lower magnetoresistive films, and further guided through the magnetically sensitive parts 61 and 62 to the magnetic bands 51' and 52' for magnetic flux guide.

この時、分岐点dにおいては、上層および下層の磁気抵
抗効果膜51.52が互いに同一材質で、膜厚および形
状も同じなのでほぼ同量の信号磁束が分岐され、感磁部
61,62に侵入することになる。そして、感磁部61
および62において、当該信号磁束により感磁部61お
よび62の抵抗が磁気抵抗効果で各々変化するのを利用
して、電流導入線91および92から各々の抵抗変化に
対応した電圧変化を検出し、さらに各々の8力電圧を差
動増幅することで磁気記録媒体7上に記録された信号を
読み取ることができる。
At this time, at the branch point d, since the upper layer and the lower layer magnetoresistive films 51 and 52 are made of the same material and have the same film thickness and shape, almost the same amount of signal magnetic flux is branched to the magnetically sensitive parts 61 and 62. There will be an intrusion. And the magnetic sensing part 61
and 62, detecting a voltage change corresponding to each resistance change from the current introduction lines 91 and 92 by utilizing the fact that the resistance of the magnetic sensing parts 61 and 62 changes due to the magnetoresistive effect due to the signal magnetic flux, Furthermore, the signals recorded on the magnetic recording medium 7 can be read by differentially amplifying the respective 8-power voltages.

この際、上層および下層の磁気抵抗効果膜51゜52に
互いに同一方向で、同意の検出電流を流すことにより、
各磁気抵抗効果膜中の磁化の向きを互いに逆向きにさせ
るような同等の相互バイアス磁界が働き、差動増幅が可
能となる。また、感磁部61および62における抵抗変
化量は、上述したように同量の信号磁束が感磁部61お
よび62に入るので同等であり、したがって感磁部61
゜62の各抵抗変化に対応した、電流導入線91および
92で検出される電圧変化量を同等である。
At this time, by passing the same detection current through the upper and lower magnetoresistive films 51 and 52 in the same direction,
Equivalent mutual bias magnetic fields act to reverse the directions of magnetization in each magnetoresistive film, making differential amplification possible. Further, the amount of resistance change in the magnetically sensitive parts 61 and 62 is the same since the same amount of signal magnetic flux enters the magnetically sensitive parts 61 and 62 as described above.
The amount of voltage change detected in the current introduction lines 91 and 92 corresponding to each resistance change of 62 degrees is equivalent.

さらに、媒体対向面8の磁気抵抗効果膜51゜52の突
出部から同時に吸い込まれた信号磁束は、各々の感磁部
61および62へ同時に到達する。
Further, the signal magnetic fluxes simultaneously sucked in from the protrusions of the magnetoresistive films 51 and 52 on the medium facing surface 8 reach the respective magnetically sensitive parts 61 and 62 simultaneously.

このため、電流導入線91および92で検出される各電
圧変化の位相も同じく1位相差が生じることはない。
Therefore, the phases of each voltage change detected by the current introduction lines 91 and 92 also do not have a one phase difference.

本実施例によれば、実施例1で述べたと同様の効果に加
えて、上述したように同量の信号磁束を同時に上層およ
び下層の磁気抵抗効果膜の感磁部へ導くことができるの
で、上層および下層の感磁部の出力電圧を差動増幅した
場合でも差動波形が歪まず、高出力が得られるという効
果がある。
According to this embodiment, in addition to the same effect as described in Embodiment 1, it is possible to simultaneously guide the same amount of signal magnetic flux to the magnetically sensitive parts of the upper and lower magnetoresistive films as described above. Even when the output voltages of the upper and lower magnetically sensitive parts are differentially amplified, the differential waveform is not distorted and a high output can be obtained.

実施例3 第3図に本発明の他の実施例による磁気抵抗効果素子の
断面図を示す。第3図の断面図は実施例2の第2図(c
、)で示した断面図に対応するものである1本実施例は
、実施例2の磁気抵抗効果素子18における上層および
下層の磁気抵抗効果膜51.52の両端部に形成した検
出電流導入線91.92のいずれか一方の端部に形成し
た上下の検出電流導入線を、−本の共通の電流導入線で
共用させた構成としたものである。その他の構成は実施
例2の場合と同様であり、その動作および効果は実施例
2の場合と全く同様である。
Embodiment 3 FIG. 3 shows a sectional view of a magnetoresistive element according to another embodiment of the present invention. The cross-sectional view in FIG. 3 is the same as in FIG. 2 (c
This embodiment corresponds to the cross-sectional views shown in , ), and shows detection current lead-in lines formed at both ends of the upper and lower magnetoresistive films 51 and 52 in the magnetoresistive element 18 of embodiment 2. The upper and lower detection current lead-in lines formed at either end of the 91 and 92 are shared by a common current lead-in line. The other configurations are the same as in the second embodiment, and the operation and effects are completely the same as in the second embodiment.

〔発明の効果〕〔Effect of the invention〕

本発明によれば、磁気記録媒体から漏れ出る信号磁束を
、その量を減少されることなく磁気抵抗効果素子の感磁
部に導くことがき、磁気抵抗効果素子の出力を高める効
果が得られる。さらにまた、2層とした磁気抵抗効果素
子の感磁部に同時間で同量の信号磁束量を導くことがで
きるので、当該感磁部の出力電圧を差動増幅した場合で
も差動波形を歪ませないという効果がある。したがって
、磁気抵抗効果素子の高出力化がさらに可能となり、狭
トラツク記録再生に適した磁気抵抗効果素子の作製が可
能である。
According to the present invention, the signal magnetic flux leaking from the magnetic recording medium can be guided to the magnetically sensitive part of the magnetoresistive element without its amount being reduced, thereby achieving the effect of increasing the output of the magnetoresistive element. Furthermore, since the same amount of signal magnetic flux can be guided to the magnetic sensing part of the two-layered magnetoresistive element at the same time, even when the output voltage of the magnetic sensing part is differentially amplified, the differential waveform can be maintained. It has the effect of not causing distortion. Therefore, it is possible to further increase the output of the magnetoresistive element, and it is possible to manufacture a magnetoresistive element suitable for narrow track recording and reproduction.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図(a)、(b)は本発明の一実施例の素子正面図
および断面図、第2図(a)、(b)。 (c)は本発明の他の実施例の素子正面図および断面図
、第3図は本発明のさらに他の実施例の素子断面図であ
る。 1・・・基板、2,4,10.15・・・絶縁層、3・
・・導電体層、5・・・磁気抵抗効果膜、6・・・感磁
部、7・・・磁気記録媒体、9・・・検出電流導入線、
11・・・上部磁気シールド層、12.18・・・磁気
抵抗効果素子、13・・・信号磁束。
FIGS. 1(a) and 1(b) are a front view and a sectional view of an element according to an embodiment of the present invention, and FIGS. 2(a) and 2(b). (c) is a front view and a sectional view of an element of another embodiment of the present invention, and FIG. 3 is a sectional view of an element of still another embodiment of the invention. 1... Substrate, 2, 4, 10.15... Insulating layer, 3.
... Conductor layer, 5... Magnetoresistive film, 6... Magnetically sensitive part, 7... Magnetic recording medium, 9... Detection current introduction line,
11... Upper magnetic shield layer, 12.18... Magnetoresistive element, 13... Signal magnetic flux.

Claims (1)

【特許請求の範囲】 1、磁気記録媒体からの信号磁界を強磁性体薄膜の磁気
抵抗効果を利用して読み取る磁気抵抗効果素子において
、該磁気抵抗効果素子に使用する上記強磁性体薄膜から
なる磁気抵抗効果膜の形状を、その中心部で磁気記録媒
体上に記録された信号の記録トラック幅に対応する感磁
部分だけ媒体対向面に突出させ、その他の残りの磁気抵
抗効果膜上に検出電流導入用のリード線を設けたことを
特徴とする磁気抵抗効果素子。 2、上記磁気抵抗効果膜を絶縁層を介した2層として下
層の磁気抵抗効果膜にも同様の電流導入用のリード線を
設け、ただし媒体対向面とその近傍の上記突出部におい
ては絶縁層を除いて上層および下層の磁気抵抗効果膜を
互いに接触させた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、上記2層の磁気抵抗効果膜上の右端部あるいは左端
部上に形成した、いずれか一方の上下の検出電流導入用
のリード線を互いに短絡させ、磁気記録媒体からの信号
磁界による上層および下層の磁気抵抗効果膜の抵抗変化
に対応した出力電圧を差動増幅して読み取ることを特徴
とした特許請求の範囲第2項記載の磁気抵抗効果素子。
[Claims] 1. A magnetoresistive element that reads a signal magnetic field from a magnetic recording medium using the magnetoresistive effect of a ferromagnetic thin film, comprising the above-mentioned ferromagnetic thin film used in the magnetoresistive element. The shape of the magnetoresistive film is such that only the magnetically sensitive part corresponding to the recording track width of the signal recorded on the magnetic recording medium at its center protrudes to the surface facing the medium, and the remaining magnetoresistive film is detected. A magnetoresistive element characterized by being provided with a lead wire for introducing current. 2. The magnetoresistive film is made of two layers with an insulating layer in between, and the lower magnetoresistive film is also provided with a similar lead wire for introducing current. Claim 1 characterized in that the upper layer and the lower layer magnetoresistive film are in contact with each other except for
The magnetoresistance effect element described in . 3. Short-circuit the upper and lower detection current lead wires formed on the right end or left end of the two layers of magnetoresistive films to each other, so that the signal magnetic field from the magnetic recording medium causes the upper layer and 3. The magnetoresistive element according to claim 2, wherein an output voltage corresponding to a change in resistance of an underlying magnetoresistive film is differentially amplified and read.
JP63283594A 1988-11-11 1988-11-11 Magneto-resistance effect element Pending JPH02130712A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63283594A JPH02130712A (en) 1988-11-11 1988-11-11 Magneto-resistance effect element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63283594A JPH02130712A (en) 1988-11-11 1988-11-11 Magneto-resistance effect element

Publications (1)

Publication Number Publication Date
JPH02130712A true JPH02130712A (en) 1990-05-18

Family

ID=17667526

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63283594A Pending JPH02130712A (en) 1988-11-11 1988-11-11 Magneto-resistance effect element

Country Status (1)

Country Link
JP (1) JPH02130712A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0675371A2 (en) * 1994-03-31 1995-10-04 Yamaha Corporation Magnetic head having magnetoresistive sensor
KR100455296B1 (en) * 2002-05-15 2004-11-06 삼성전자주식회사 A magnetic reading head

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0675371A2 (en) * 1994-03-31 1995-10-04 Yamaha Corporation Magnetic head having magnetoresistive sensor
EP0675371A3 (en) * 1994-03-31 1995-12-27 Yamaha Corp Magnetic head having magnetoresistive sensor.
KR100455296B1 (en) * 2002-05-15 2004-11-06 삼성전자주식회사 A magnetic reading head

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