JPH04285712A - Magneto-resistance effect type head - Google Patents
Magneto-resistance effect type headInfo
- Publication number
- JPH04285712A JPH04285712A JP4840391A JP4840391A JPH04285712A JP H04285712 A JPH04285712 A JP H04285712A JP 4840391 A JP4840391 A JP 4840391A JP 4840391 A JP4840391 A JP 4840391A JP H04285712 A JPH04285712 A JP H04285712A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- gap
- magneto
- recording medium
- resistance effect
- 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.)
- Withdrawn
Links
- 230000000694 effects Effects 0.000 title abstract description 6
- 239000004020 conductor Substances 0.000 claims abstract description 9
- 239000000696 magnetic material Substances 0.000 claims abstract description 8
- 230000035699 permeability Effects 0.000 claims abstract description 8
- 230000004907 flux Effects 0.000 description 7
- 239000010408 film Substances 0.000 description 4
- 229910000889 permalloy Inorganic materials 0.000 description 3
- 239000000463 material Substances 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 238000001514 detection method Methods 0.000 description 1
- 239000011810 insulating material Substances 0.000 description 1
- 238000007747 plating Methods 0.000 description 1
- 239000000758 substrate Substances 0.000 description 1
- 239000010409 thin film Substances 0.000 description 1
Classifications
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B5/00—Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
- G11B5/127—Structure or manufacture of heads, e.g. inductive
- G11B5/33—Structure or manufacture of flux-sensitive heads, i.e. for reproduction only; Combination of such heads with means for recording or erasing only
- G11B5/39—Structure 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
- G11B5/3903—Structure 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
- G11B5/3906—Details related to the use of magnetic thin film layers or to their effects
- G11B5/3916—Arrangements in which the active read-out elements are coupled to the magnetic flux of the track by at least one magnetic thin film flux guide
- G11B5/3919—Arrangements in which the active read-out elements are coupled to the magnetic flux of the track by at least one magnetic thin film flux guide the guide being interposed in the flux path
- G11B5/3922—Arrangements in which the active read-out elements are coupled to the magnetic flux of the track by at least one magnetic thin film flux guide the guide being interposed in the flux path the read-out elements being disposed in magnetic shunt relative to at least two parts of the flux guide structure
- G11B5/3925—Arrangements in which the active read-out elements are coupled to the magnetic flux of the track by at least one magnetic thin film flux guide the guide being interposed in the flux path the read-out elements being disposed in magnetic shunt relative to at least two parts of the flux guide structure the two parts being thin films
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B5/00—Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
- G11B5/127—Structure or manufacture of heads, e.g. inductive
- G11B5/33—Structure or manufacture of flux-sensitive heads, i.e. for reproduction only; Combination of such heads with means for recording or erasing only
- G11B5/39—Structure 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
- G11B5/3903—Structure 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
- G11B5/3967—Composite structural arrangements of transducers, e.g. inductive write and magnetoresistive read
Landscapes
- Engineering & Computer Science (AREA)
- Manufacturing & Machinery (AREA)
- Magnetic Heads (AREA)
Abstract
Description
【0001】0001
【産業上の利用分野】本発明は、磁気ディスク装置等に
用いられ、記録再生を行なうヨーク型磁気抵抗効果型ヘ
ッドに関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a yoke-type magnetoresistive head used in magnetic disk drives and the like for recording and reproducing.
【0002】0002
【従来の技術】図2(A),(B)には従来のヨーク型
MRヘッドの一例の平面図,断面図を示す。上部ヨーク
11a,11b,下部ヨーク12は、膜厚3μm程度の
パーマロイ膜で作製されており、磁気記録媒体からの信
号磁界をMR素子13に導くための磁束導入路として機
能している。磁気抵抗効果(MR)素子13は、膜厚1
000Å程度の高透率磁性材料のパーマロイ膜で形成さ
れており、上部ヨーク11a,11bとは絶縁されてい
る。再生時に記録媒体からの信号磁束の検出は、MR素
子13の両端に設置したリード線14にセンス電流を流
し、MR素子13の両端に発生する電圧の変化を取り出
すことにより行なっている。また、導体コイル15に記
録媒体の記録情報を消去しないような微弱な電流を流す
ことによって所望のバイアス磁界を発生させ、これをM
R素子13に印加し、MR素子13の動作点を線型性の
良い点に移動させている。また、MR素子に効率よく磁
束を通過させるために、上部ヨークMR素子13上には
空隙16か設けられている。また、記録を行なうには、
導体コイル15に電流を流し、上部ヨーク11aと下部
ヨーク12間のギャップの発生磁界で記録媒体へ信号を
記録する。2. Description of the Related Art FIGS. 2A and 2B show a plan view and a sectional view of an example of a conventional yoke type MR head. The upper yokes 11a, 11b and the lower yoke 12 are made of a permalloy film with a thickness of about 3 μm, and function as a magnetic flux introducing path for guiding the signal magnetic field from the magnetic recording medium to the MR element 13. The magnetoresistive (MR) element 13 has a film thickness of 1
It is formed of a permalloy film of a highly permeable magnetic material with a thickness of approximately 0.000 Å, and is insulated from the upper yokes 11a and 11b. Detection of signal magnetic flux from the recording medium during reproduction is performed by passing a sense current through lead wires 14 installed at both ends of the MR element 13 and extracting changes in voltage generated at both ends of the MR element 13. In addition, a desired bias magnetic field is generated by passing a weak current that does not erase recorded information on the recording medium through the conductor coil 15, and this is applied to the M
The voltage is applied to the R element 13 to move the operating point of the MR element 13 to a point with good linearity. Further, a gap 16 is provided above the upper yoke MR element 13 in order to efficiently pass the magnetic flux through the MR element. Also, to record,
A current is passed through the conductor coil 15, and a signal is recorded on the recording medium by the magnetic field generated in the gap between the upper yoke 11a and the lower yoke 12.
【0003】0003
【発明が解決しようとする課題】しかし、従来のヨーク
型MRヘッドを記録のために使用した場合、上部ヨーク
11a,11b間に設けられた空隙16が大きな磁気抵
抗となるために、記録媒体を飽和記録するのに充分なヘ
ッド発生磁界が得られないという問題を有していた。従
って、保磁力の比較的小さい媒体しか記録できないか、
またはヨーク型MRヘッドは再生専用として用いられ、
記録用として別個の薄膜ヘッドを作製する必要があった
。However, when a conventional yoke-type MR head is used for recording, the air gap 16 provided between the upper yokes 11a and 11b creates a large magnetic resistance, making it difficult to hold the recording medium. There was a problem in that a head-generated magnetic field sufficient for saturation recording could not be obtained. Therefore, only media with relatively small coercive force can be recorded, or
Alternatively, a yoke type MR head is used only for reproduction.
It was necessary to create a separate thin film head for recording.
【0004】本発明は上記の点に鑑みなされたもので、
従来通りの再生出力を得ると共に、記録媒体を飽和記録
するに充分な磁界を発生できる磁気抵抗効果型ヘッドを
提供することを目的とする。[0004] The present invention has been made in view of the above points.
It is an object of the present invention to provide a magnetoresistive head that can generate a magnetic field sufficient to saturate recording on a recording medium while obtaining a conventional reproduction output.
【0005】[0005]
【課題を解決するための手段】本発明の磁気抵抗効果型
ヘッドは、磁気記録媒体からの信号磁界をヨークの形成
するギャップにより、検出してヨークの空隙部に設けら
れた磁気抵抗効果素子に導き信号再生を行ない、かつ導
体コイルに通電して発生した磁界をヨークによりギャッ
プに導き磁気記録媒体に記録する磁気抵抗効果型ヘッド
において、磁気抵抗効果素子を設けたヨークの空隙部に
磁気抵抗効果素子より充分に低い透磁率を持つ磁性体を
設ける。[Means for Solving the Problems] A magnetoresistive head of the present invention detects a signal magnetic field from a magnetic recording medium using a gap formed by a yoke, and transmits the signal to a magnetoresistive element provided in a gap of the yoke. In a magnetoresistive head that reproduces guided signals and guides the magnetic field generated by energizing a conductor coil to a gap using a yoke to record on a magnetic recording medium, the magnetoresistive effect is applied to the gap in the yoke in which the magnetoresistive element is provided. A magnetic material having a sufficiently lower magnetic permeability than the element is provided.
【0006】[0006]
【作用】本発明においては、空隙部に形成された磁性体
は磁気抵抗効果型素子よりも充分に透磁率が低いため再
生磁束はヨークからほとんど磁気抵抗効果素子に流れ従
来通りの再生出力が得られる。また記録時には導体コイ
ルの通電により発生した磁束が磁性体を通り、ギャップ
に記録媒体の飽和記録と充分な磁界が得られる。[Operation] In the present invention, since the magnetic material formed in the gap has sufficiently lower magnetic permeability than the magnetoresistive element, most of the reproduction magnetic flux flows from the yoke to the magnetoresistive element, and the reproduction output as before can be obtained. It will be done. Further, during recording, the magnetic flux generated by energizing the conductor coil passes through the magnetic material, so that saturation recording of the recording medium and a sufficient magnetic field can be obtained in the gap.
【0007】[0007]
【実施例】図1,図2は夫々本発明のヘッドの一実施例
の平面図,断面拡大図を示す。両図中、図3と同一部分
には同一符号を付す。DESCRIPTION OF THE PREFERRED EMBODIMENTS FIGS. 1 and 2 show a plan view and an enlarged sectional view of an embodiment of the head of the present invention, respectively. In both figures, the same parts as in FIG. 3 are given the same reference numerals.
【0008】図1,図2において基板17上には下部ヨ
ーク12が形成され、下部ヨーク12上には絶縁材料の
ギャップ層18を介して上部ヨーク11aが形成される
と共に下部ヨーク12と接触して上部ヨーク11bが形
成されている。In FIGS. 1 and 2, a lower yoke 12 is formed on a substrate 17, and an upper yoke 11a is formed on the lower yoke 12 with a gap layer 18 of an insulating material interposed therebetween, and is in contact with the lower yoke 12. An upper yoke 11b is formed.
【0009】上部ヨーク11a,11bと下部ヨーク1
2とで囲まれる空間は絶縁層19が形成され、絶縁層1
9内を導体コイル15が挿通されて巻回されている。絶
縁層19上には上部ヨーク11a,11bで形成される
空隙16内にパーマロイ膜のMR素子13が形成されて
おり、MR素子13は絶縁膜20によって上部ヨーク1
1a,11b夫々と絶縁されている。Upper yokes 11a, 11b and lower yoke 1
Insulating layer 19 is formed in the space surrounded by insulating layer 1 and
A conductor coil 15 is inserted through and wound inside the coil 9 . An MR element 13 made of a permalloy film is formed on the insulating layer 19 in a gap 16 formed by the upper yokes 11a and 11b.
1a and 11b are insulated from each other.
【0010】また、空隙16内には例えばマスクメッキ
法又はリフトオフ法等により磁性体層21が形成されて
いる。磁性体層21の透磁率は数百程度とMR素子13
に比して充分に低い材料、つまり磁気異方性磁界Hk
がMR素子13に比して充分に大きい材料で形成されて
いる。A magnetic layer 21 is formed within the gap 16 by, for example, a mask plating method or a lift-off method. The magnetic permeability of the magnetic layer 21 is about several hundreds, and the MR element 13
Materials with sufficiently low magnetic anisotropy field Hk compared to
is made of a material that is sufficiently larger than the MR element 13.
【0011】ここで、再生時には記録媒体から発生する
微弱な信号磁界による再生磁束は透磁率が低い磁性体に
はほとんど流入することなく高透磁率のMR素子13に
流入し、従来通りの再生出力が得られる。[0011] During reproduction, the reproduction magnetic flux due to the weak signal magnetic field generated from the recording medium hardly flows into the magnetic material with low magnetic permeability, but instead flows into the MR element 13 with high magnetic permeability, resulting in the conventional reproduction output. is obtained.
【0012】記録時には導体コイル15に電流を流すこ
とにより上部ヨーク11a,11b間の空隙16には磁
性体21の磁気異方性磁界Hk を越える磁界が加わり
磁束が磁性体21内を通るため、上部ヨーク11aと下
部ヨーク12との間のギャップには記録媒体を飽和記録
させるに充分大きなヘッド発生磁界が得られる。During recording, by passing a current through the conductor coil 15, a magnetic field exceeding the magnetic anisotropy field Hk of the magnetic body 21 is applied to the air gap 16 between the upper yokes 11a and 11b, and magnetic flux passes through the inside of the magnetic body 21. In the gap between the upper yoke 11a and the lower yoke 12, a head-generated magnetic field large enough to saturate the recording medium can be obtained.
【0013】[0013]
【発明の効果】上述の如く、本発明の磁気抵抗効果型ヘ
ッドによれば、従来通りの再生出力を得ると共に、記録
媒体を飽和記録するに充分な磁界を発生できる。As described above, according to the magnetoresistive head of the present invention, it is possible to obtain a conventional reproduction output and generate a magnetic field sufficient to saturate recording on a recording medium.
【図1】本発明ヘッドの一実施例の平面図である。FIG. 1 is a plan view of an embodiment of the head of the present invention.
【図2】図1のヘッドの断面拡大図である。FIG. 2 is an enlarged cross-sectional view of the head in FIG. 1;
【図3】従来ヘッドの一例の平面図,断面図である。FIG. 3 is a plan view and a sectional view of an example of a conventional head.
11a,11b 上部ヨーク 12 下部ヨーク 13 MR素子 15 導体コイル 16 空隙 21 磁性体 11a, 11b Upper yoke 12 Lower yoke 13 MR element 15 Conductor coil 16 Voids 21 Magnetic material
Claims (1)
(11a,11b,12)の形成するギャップにより、
検出して該ヨークの空隙部(16)に設けられた磁気抵
抗効果素子に導き信号再生を行ない、かつ導体コイル(
15)に通電して発生した磁界を該ヨーク(11a,1
1b,12)により該ギャップに導き磁気記録媒体に記
録する磁気抵抗効果型ヘッドにおいて、該磁気抵抗効果
素子(13)を設けたヨークの空隙部(16)に該磁気
抵抗効果素子(13)より充分に低い透磁率を持つ磁性
体(21)を設けたことを特徴とする磁気抵抗効果型ヘ
ッド。Claim 1: A signal magnetic field from a magnetic recording medium is transmitted through a gap formed by a yoke (11a, 11b, 12).
The signal is detected and guided to the magnetoresistive element provided in the gap (16) of the yoke for signal reproduction, and the conductor coil (
The magnetic field generated by energizing the yokes (11a, 15)
1b, 12) in which the magnetoresistive element (13) is guided into the gap to record on the magnetic recording medium, the magnetoresistive element (13) enters the gap (16) of the yoke in which the magnetoresistive element (13) is provided. A magnetoresistive head characterized by being provided with a magnetic material (21) having sufficiently low magnetic permeability.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP4840391A JPH04285712A (en) | 1991-03-13 | 1991-03-13 | Magneto-resistance effect type head |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP4840391A JPH04285712A (en) | 1991-03-13 | 1991-03-13 | Magneto-resistance effect type head |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH04285712A true JPH04285712A (en) | 1992-10-09 |
Family
ID=12802340
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP4840391A Withdrawn JPH04285712A (en) | 1991-03-13 | 1991-03-13 | Magneto-resistance effect type head |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH04285712A (en) |
-
1991
- 1991-03-13 JP JP4840391A patent/JPH04285712A/en not_active Withdrawn
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Legal Events
Date | Code | Title | Description |
---|---|---|---|
A300 | Application deemed to be withdrawn because no request for examination was validly filed |
Free format text: JAPANESE INTERMEDIATE CODE: A300 Effective date: 19980514 |