JPH0438614A - Magneto-resistance effect element and its applied magnetic head and recording and reproducing device - Google Patents
Magneto-resistance effect element and its applied magnetic head and recording and reproducing deviceInfo
- Publication number
- JPH0438614A JPH0438614A JP14126590A JP14126590A JPH0438614A JP H0438614 A JPH0438614 A JP H0438614A JP 14126590 A JP14126590 A JP 14126590A JP 14126590 A JP14126590 A JP 14126590A JP H0438614 A JPH0438614 A JP H0438614A
- Authority
- JP
- Japan
- Prior art keywords
- magnetoresistive
- film
- magnetoresistive film
- conductor
- magnetoresistive element
- 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
Links
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
- G11B5/3945—Heads comprising more than one sensitive element
- G11B5/3948—Heads comprising more than one sensitive element the sensitive elements being active read-out elements
- G11B5/3958—Heads comprising more than one sensitive element the sensitive elements being active read-out elements the active elements being arranged in a single plane, e.g. "matrix" disposition
- G11B5/3961—Heads comprising more than one sensitive element the sensitive elements being active read-out elements the active elements being arranged in a single plane, e.g. "matrix" disposition disposed at an angle to the direction of the track or relative movement
- G11B5/3964—Heads comprising more than one sensitive element the sensitive elements being active read-out elements the active elements being arranged in a single plane, e.g. "matrix" disposition disposed at an angle to the direction of the track or relative movement for transducing on a single track
Landscapes
- Physics & Mathematics (AREA)
- Mathematical Physics (AREA)
- Engineering & Computer Science (AREA)
- Manufacturing & Machinery (AREA)
- Magnetic Heads (AREA)
Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は、磁気記録媒体に記録された情報を読取るため
の専用の感磁素子に係り、さらに詳しくは強磁性体膜の
磁気抵抗効果を利用した高感度の磁気抵抗効果型の感磁
素子およびそれを用いた磁気ヘッドならびに磁気記録再
生装置に関する。[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a dedicated magneto-sensitive element for reading information recorded on a magnetic recording medium, and more specifically, to a magneto-sensitive element for reading information recorded on a magnetic recording medium. The present invention relates to a highly sensitive magnetoresistive magnetic sensing element, a magnetic head using the same, and a magnetic recording/reproducing device.
従来の例えば、バイアス磁界印加手段として軟磁性体膜
を用いた磁気抵抗効果素子は、特開昭50−65213
号公報において記載されているように、磁気抵抗効果膜
の両端部に2本の導体部を設けた構成になっており、こ
の形式の磁気抵抗効果素子の出力は、外部磁界に対して
放物線的な出力を示すものである。一方、特開昭61−
199684号公報には、ダイナミックレンジの拡大と
雑音の低減等を目的とした磁気抵抗効果素子が提案され
ており、これは上記特開昭50−65213号公報記載
の放物線的な出力をもつ2つの磁気抵抗効果素子の出力
を、差動化させた構成の軟磁性体を用いたバイアス型の
磁気抵抗効果素子である。この磁気抵抗効果素子は、差
動化させるために磁気抵抗効果膜の中央部に共通の導体
部を設け、さらに上記磁気抵抗効果膜の両端部に設けら
れている2本の導体部とを合わせて、計3本の導体部を
設けた構成の磁気抵抗効果素子である。For example, a conventional magnetoresistive element using a soft magnetic film as a bias magnetic field applying means is disclosed in Japanese Patent Application Laid-Open No. 50-65213.
As described in the publication, the structure is such that two conductor parts are provided at both ends of the magnetoresistive film, and the output of this type of magnetoresistive element is parabolic in response to an external magnetic field. This shows the output. On the other hand, JP-A-61-
No. 199684 proposes a magnetoresistive element for the purpose of expanding the dynamic range and reducing noise. This is a bias-type magnetoresistive element using a soft magnetic material in which the output of the magnetoresistive element is differentiated. This magnetoresistive element has a common conductor part provided in the center of the magnetoresistive film in order to make a differential signal, and a common conductor part provided at both ends of the magnetoresistive film. This is a magnetoresistive element having a configuration in which a total of three conductor parts are provided.
磁気記録密度の増加の要求にともなって記録トラック幅
も減少させる必要が生じる。上述した従来技術である特
開昭50−65213号公報に記載されている磁気抵抗
効果素子は、導体部が2本であるため狭トラック化され
た磁気記録媒体に対しては有利であるが、出力が放物線
的であるためにダイナミツトレンジが狭いという欠点が
あった。With the demand for increased magnetic recording density, it is also necessary to reduce the recording track width. The magnetoresistive element described in Japanese Patent Application Laid-Open No. 50-65213, which is the prior art mentioned above, has two conductor parts, so it is advantageous for magnetic recording media with narrow tracks. The drawback was that the dynamic range was narrow because the output was parabolic.
一方、従来の特開昭61−199684号公報に4一
記載の差動型の磁気抵抗効果素子においては、ダイナミ
ックレンジが広いという点では有利であるが、磁気記録
媒体の狭トラック化が進むにつれて、それに対応した3
本の導体部を有する磁気抵抗効果素子を作製することは
、特に磁気抵抗効果膜の中央に接続される導体部の幅を
小さくする必要があって、これはパターニング精度、エ
レクトロマイグレーションなどの点から言って極めて困
難であるという問題があった。また、両者共通の問題点
として、狭トラック化すると磁気抵抗効果膜中の電流密
度分布が素子の再生出力に影響を与えると言うことがあ
った。On the other hand, the conventional differential type magnetoresistive element described in 41 of JP-A-61-199684 is advantageous in that it has a wide dynamic range, but as the tracks of magnetic recording media become narrower, , the corresponding 3
In order to manufacture a magnetoresistive element having a conductor part, it is necessary to reduce the width of the conductor part connected to the center of the magnetoresistive film, and this is necessary from the viewpoint of patterning accuracy, electromigration, etc. The problem was that it was extremely difficult. Further, a problem common to both is that when the track is made narrower, the current density distribution in the magnetoresistive film affects the reproduction output of the element.
本発明の目的は、上記従来技術における問題点を解消す
るものであって、高密度磁気記録媒体の狭トラック化に
対応した3本の導体部を有する磁気抵抗効果素子を構成
し、かつ差動型の素子出力が得られ、ダイナミックレン
ジの広い磁気抵抗効果素子およびそれを用いた磁気ヘッ
ドならびに磁気記録再生装置を提供することにある。An object of the present invention is to solve the above-mentioned problems in the prior art, and to configure a magnetoresistive element having three conductor parts corresponding to narrower tracks of high-density magnetic recording media, and An object of the present invention is to provide a magnetoresistive element that can obtain a type of element output and has a wide dynamic range, a magnetic head using the same, and a magnetic recording/reproducing device.
〔課題を解決するための手段〕
上記本発明の目的を達成するために、磁気抵抗効果素子
に接続した導体に流れる信号検出電流の方向が、少なく
とも磁気抵抗効果膜の上では磁気記録媒体のトラック幅
方向にほぼ平行となるように構成する。すなわち、具体
的には磁気抵抗効果素子を差動化させるために設けた磁
気抵抗効果膜の中央部に設ける共通の導体部を、少なく
とも磁気抵抗効果膜の上においてはトラック幅方向にほ
ぼ平行となるように形成することにより本発明の磁気抵
抗効果素子を実現することができる。[Means for Solving the Problems] In order to achieve the above-mentioned object of the present invention, the direction of the signal detection current flowing through the conductor connected to the magnetoresistive element is set so that the direction of the signal detection current flowing through the conductor connected to the magnetoresistive element is aligned with the track of the magnetic recording medium at least on the magnetoresistive film It is configured to be approximately parallel to the width direction. Specifically, the common conductor section provided in the center of the magnetoresistive film provided to differentiate the magnetoresistive element is arranged substantially parallel to the track width direction at least on the magnetoresistive film. The magnetoresistive element of the present invention can be realized by forming the magnetoresistive element as follows.
磁気抵抗効果素子を差動化させるために設けた磁気抵抗
効果膜の中央部の導体を、磁気抵抗効果膜上に平行に設
けることにより、導体部と磁気抵抗効果膜の接続部付近
では、検出電流の密度分布が磁気抵抗効果膜の全面で均
一となる。これにより、媒体からの磁界信号が磁気抵抗
効果膜に加わったとき、上記膜全面で磁化の向きが変化
するため、狭トラック化を行っても検出電流の電流密度
分布による再生出力の低下を抑制することができる。By placing the conductor in the center of the magnetoresistive film, which is provided to make the magnetoresistive element differential, in parallel to the magnetoresistive film, detection is possible near the connection between the conductor and the magnetoresistive film. The current density distribution becomes uniform over the entire surface of the magnetoresistive film. As a result, when a magnetic field signal from the medium is applied to the magnetoresistive film, the direction of magnetization changes over the entire surface of the film, so even if the track is made narrower, the reduction in reproduction output due to the current density distribution of the detection current is suppressed. can do.
また、磁気抵抗効果膜上に形成された導体部はスルーホ
ールから右側と左側では、それぞれ逆向きのバイアス磁
界を発生する。この逆向きのバイアス磁界により、中央
から左側の磁気抵抗効果膜と右側の磁気抵抗効果膜の電
圧変化が磁界0(ゼロ)のときのバイアス点を基準にし
て、磁気記録媒体からの信号磁界に対して増加あるいは
減少するように作用する。その結果、両者を合成した磁
気抵抗効果膜全体の電圧変化は、差動化させたときに得
られる電圧変化と同様の変化を示すことになる。Further, the conductor portion formed on the magnetoresistive film generates bias magnetic fields in opposite directions on the right side and left side of the through hole, respectively. Due to this bias magnetic field in the opposite direction, the voltage change of the magnetoresistive film on the left side and the magnetoresistive film on the right side of the center changes to the signal magnetic field from the magnetic recording medium with reference to the bias point when the magnetic field is 0 (zero). It acts to increase or decrease. As a result, the voltage change of the entire magnetoresistive film in which both are combined exhibits a voltage change similar to the voltage change obtained when differentialization is performed.
以下に本発明の一実施例を挙げ、図面に基づいてさらに
詳細に説明する。An embodiment of the present invention will be described below in more detail based on the drawings.
(実施例 1)
第1図は、本実施例において例示する磁気抵抗効果素子
の構成の概略を示す斜視図で、第2図(a)は本実施例
における磁気抵抗効果素子の構成の一例を示す平面図で
、第2図(b)は第2図(、)のA−A断面図である。(Example 1) FIG. 1 is a perspective view showing an outline of the configuration of a magnetoresistive element exemplified in this example, and FIG. 2(a) is an example of the configuration of a magnetoresistive element in this example. 2(b) is a sectional view taken along the line AA in FIG. 2(,).
本実施例においては、基板1上にN i −F e合金
などの軟磁性体膜よりなる磁気シールド2を0.5〜3
μmの厚さに、真空蒸着法やスパッタ法などの手段で積
層し、ホトリソグラフィの手法により、所定の形状にパ
ターニングした。その上に、絶縁層3となるSin、や
AQ203を0.05〜0.5μmの厚さに、スパッタ
法を用いて積層した。In this embodiment, a magnetic shield 2 made of a soft magnetic material film such as a Ni-Fe alloy is placed on a substrate 1 with a thickness of 0.5 to 3
The layers were laminated to a thickness of μm by means such as vacuum evaporation or sputtering, and patterned into a predetermined shape by photolithography. On top of that, a layer of Sin or AQ203 to form the insulating layer 3 was laminated to a thickness of 0.05 to 0.5 μm using a sputtering method.
磁気抵抗効果膜4となるNi−Fe合金などを真空蒸着
法やスパッタ法などを用いて絶縁層3の上に積層した後
、ホトリソグラフィの手法により所定の形状にパターニ
ングした。なお、磁気抵抗効果膜3としてはNi−Fe
合金のほかに、例えばN i −G o合金など磁気抵
抗効果をもつ他の合金系材料を使用してもなんら差し支
えない。そして、引き続き磁気抵抗効果膜4の端部に検
出電流を流すための導体部5を、Cuなどの良導体を用
いて積層しホトリソグラフィの手法によりパターニング
して作製した。ここで、2本の導体部5の間隔すなわち
トラック幅は5μmとした。また、導体部5の材料とし
てはCuの他にAuやAgなども好適に用いることがで
きる。A Ni--Fe alloy, etc., which will become the magnetoresistive film 4, was laminated on the insulating layer 3 using a vacuum evaporation method, a sputtering method, or the like, and then patterned into a predetermined shape using a photolithography method. Note that the magnetoresistive film 3 is made of Ni-Fe.
In addition to alloys, there is no problem in using other alloy-based materials that have a magnetoresistive effect, such as Ni-Go alloys. Subsequently, a conductor section 5 for passing a detection current through the end of the magnetoresistive film 4 was fabricated by laminating a good conductor such as Cu and patterning it by photolithography. Here, the interval between the two conductor portions 5, ie, the track width, was set to 5 μm. Furthermore, as the material for the conductor portion 5, other materials such as Au and Ag can also be suitably used in addition to Cu.
次に、絶縁層6となるSin、やAfl、03をスパッ
タ法などにより0.05〜1.0μmの厚さに積層し、
ホトリソグラフィの手法によりスルーホール7を開けた
後、磁気抵抗効果膜4の中央部から検出電流を流しバイ
アス印加手段ともなる導体部8をCuなどの良導体を用
いて積層し、ホトリソグラフィの手法により所定の形状
にパターニングすることにより作製した。ここで、スル
ーホール7より左側の磁気抵抗効果膜4と、右側の磁気
抵抗効果膜4で得られる出力波形が対称となるように、
スルーホール7の位置は磁気抵抗効果膜4の中央に設け
る必要がある。また、導体部8はバイアス印加手段とし
ても用いることができるように、磁気抵抗効果膜4の上
部または下部に平行に設ける。ここで、スルーホール7
の幅は0.8μmとした。導体部8の材料としてはCu
の他にAuやAgなども好適に用いることができる。Next, Sin, Afl, 03, which will become the insulating layer 6, is laminated to a thickness of 0.05 to 1.0 μm by sputtering or the like.
After opening a through hole 7 using a photolithography method, a conductor section 8, which also serves as a bias application means, through which a detection current is passed from the center of the magnetoresistive film 4, is laminated using a good conductor such as Cu. It was produced by patterning into a predetermined shape. Here, so that the output waveforms obtained from the magnetoresistive film 4 on the left side of the through hole 7 and the magnetoresistive film 4 on the right side are symmetrical,
The through hole 7 must be located at the center of the magnetoresistive film 4. Further, the conductor portion 8 is provided in parallel above or below the magnetoresistive film 4 so that it can also be used as a bias applying means. Here, through hole 7
The width was 0.8 μm. The material of the conductor part 8 is Cu.
In addition, Au, Ag, etc. can also be suitably used.
次に、絶縁層9となるSin、やAf1203などを0
.05〜1.0μm積層する。その上に、磁気シールド
10となるNi−Fe合金などの軟磁性体を0.5〜3
.0μm積層し、ホトリソグラフィの手法により所定の
形状にパターニングした。Next, the insulating layer 9 is made of Sin, Af1203, etc.
.. 05 to 1.0 μm lamination. On top of that, a soft magnetic material such as Ni-Fe alloy, which will become the magnetic shield 10, is applied to the
.. The layers were stacked to a thickness of 0 μm and patterned into a predetermined shape using photolithography.
さらに、導体部5.8上に検出電流導入用のパッド部1
2を、Cuなどの良導体を用いて積層することにより作
製し、最後に保護層11をSiO□やAf120.を1
0〜50μm積層することにより磁気抵抗効果素子13
を作製した。Furthermore, a pad portion 1 for introducing a detection current is placed on the conductor portion 5.8.
2 using a good conductor such as Cu, and finally a protective layer 11 made of SiO□ or Af120. 1
By laminating layers of 0 to 50 μm, the magnetoresistive element 13
was created.
次に、上述の手法で作製した磁気抵抗効果素子13の動
作について説明する。まず、パッド部12aと12b、
12cと12dの間に導体部8と5を通して、それぞれ
検出電流11.12を流す。Next, the operation of the magnetoresistive element 13 manufactured by the above method will be explained. First, pad portions 12a and 12b,
Detection currents 11 and 12 are passed between conductor portions 8 and 5 between 12c and 12d, respectively.
このとき、i□と12の大きさは等しくする。この検出
電流11.12が導体部8で作るバイアス磁界は、スル
ーホール7より左側と右側では互いに逆向きとなる。こ
の結果、両者の磁気抵抗効果膜4中の磁化の向きは、M
lおよびM2に示すように、電流11.12とは互いに
逆方向のある角度θをなす方向となる。この状態に磁気
記録媒体14からの磁界信号15が加わると、スルーホ
ール7より左側の磁気抵抗効果膜4を通して測定した電
圧変化は、信号磁界に対して第3図に示す曲線16のよ
うに+ΔVの変化を生じる。一方、右側の磁気抵抗効果
膜4を通して測定した電圧変化は、信号磁界に対して同
図に示す曲線17のように、全く180°対称の−ΔV
の変化を示すことになる。At this time, the sizes of i□ and 12 are made equal. The bias magnetic fields generated by the detection currents 11 and 12 in the conductor section 8 are in opposite directions on the left and right sides of the through hole 7. As a result, the direction of magnetization in both magnetoresistive films 4 is M
As shown by 1 and M2, the directions are opposite to the currents 11 and 12 and form a certain angle θ. When a magnetic field signal 15 from the magnetic recording medium 14 is applied to this state, the voltage change measured through the magnetoresistive film 4 on the left side of the through hole 7 is +ΔV with respect to the signal magnetic field as shown in the curve 16 shown in FIG. causes a change in On the other hand, the voltage change measured through the magnetoresistive film 4 on the right side is -ΔV, which is completely 180° symmetrical with respect to the signal magnetic field, as shown in the curve 17 shown in the figure.
This indicates a change in
そして、結局、パッド部12a〜12dより読み取られ
る、磁気抵抗効果膜全体の電圧変化ΔVは、第3図に示
す曲線18のように、信号磁界Hの正(プラス)側と負
(マイナス)側とで対称の形となり、媒体に書き込まれ
た正負の信号磁界Hは曲線18の波形に対応した出力波
形として検出することができる。In the end, the voltage change ΔV across the entire magnetoresistive film, which is read from the pad portions 12a to 12d, is on the positive (plus) side and the negative (minus) side of the signal magnetic field H, as shown by the curve 18 shown in FIG. The positive and negative signal magnetic fields H written on the medium can be detected as an output waveform corresponding to the waveform of the curve 18.
上記の本実施例において作製した磁気抵抗効果素子13
によって得られる第3図の曲線18のような出力波形は
、ちょうど従来の磁気抵抗効果膜4を差動化した磁気抵
抗効果素子によって得られる波形とほぼ同等である。す
なわち、信号磁界Hに対するダイナミックレンジを広げ
ると同時に、雑音を低減できる効果がある。さらにまた
、導体部8に流れる検出電流i□、12の方向が磁気抵
抗効果膜4の上では、トラック幅方向に平行となるため
、検出電流は磁気抵抗効果膜4の全面に均一に流れ、狭
トラック化によって生じる電流密度の分布による再生出
力の低下を防止する効果がある。Magnetoresistive element 13 produced in this example above
The output waveform obtained by the curve 18 in FIG. 3 is almost equivalent to the waveform obtained by a conventional magnetoresistive element in which the magnetoresistive film 4 is made differential. That is, there is an effect that the dynamic range for the signal magnetic field H can be expanded and at the same time noise can be reduced. Furthermore, since the direction of the detection current i□, 12 flowing through the conductor portion 8 is parallel to the track width direction on the magnetoresistive film 4, the detection current flows uniformly over the entire surface of the magnetoresistive film 4. This has the effect of preventing a reduction in reproduction output due to current density distribution caused by narrowing the track.
ここで、スルーホール7の幅とダイナミックレンジの幅
は密接な関係があり、スルーホール7の幅を2倍、3倍
と大きくするとダイナミックレンジは1/2.1/3と
減少してしまう。トラック幅が同じ2端子のヘッドと3
端子のヘッドで、ダイナミックレンジが同じになっては
差動型ヘッドを形成する意味がなくなる。そこで、スル
ーホール7の幅はできるかぎり狭くする必要がある。現
在のホトリソグラフィ技術ならば、エキシマレーザ光を
用いることにより0.5μm@のパターンを形成可能で
あり、スルーホール7の幅も0.5μmとすることがで
きる。そこで、狭トラック化しつつ、スルーホール7の
幅をトラック幅の1/2から最小0.5μmとするため
には、スルーホール7の幅とトラック幅の比は1/2〜
1/40の範囲が望ましい。Here, there is a close relationship between the width of the through hole 7 and the width of the dynamic range, and if the width of the through hole 7 is doubled or tripled, the dynamic range will be reduced to 1/2.1/3. Two terminal heads and three with the same track width
If the dynamic range of the terminal heads were to be the same, there would be no point in forming a differential head. Therefore, it is necessary to make the width of the through hole 7 as narrow as possible. With the current photolithography technology, it is possible to form a pattern of 0.5 μm@ by using excimer laser light, and the width of the through hole 7 can also be set to 0.5 μm. Therefore, in order to narrow the track and make the width of the through hole 7 from 1/2 of the track width to a minimum of 0.5 μm, the ratio of the width of the through hole 7 to the track width should be 1/2 to 0.5 μm.
A range of 1/40 is desirable.
なお、本実施例においてはバイアス印加手段として導体
部8を磁気抵抗効果膜4の上部に平行に設ける場合を示
したが、その他にシャント膜や電流線あるいは永久磁石
などを併用しても本発明の効果は変わらない。Although this embodiment shows a case in which the conductor section 8 is provided in parallel to the upper part of the magnetoresistive film 4 as a bias applying means, the present invention may also be applied in combination with a shunt film, a current line, a permanent magnet, etc. The effect remains unchanged.
また、本実施例においては磁気シールド2.10用に軟
磁性体薄膜を使用する例を挙げたが、これの代りにバル
クの軟磁性体を用いても上記と同様の効果が得られるこ
とは言うまでもない。In addition, in this example, an example is given in which a soft magnetic thin film is used for the magnetic shield 2.10, but the same effect as above can be obtained even if a bulk soft magnetic material is used instead. Needless to say.
(実施例 2)
第4図は、本実施例において例示する磁気抵抗効果素子
の構成の概略を示す斜視図である。本実施例においては
、上記実施例1で示した磁気抵抗効果素子13の導体部
5.8において、磁気抵抗効果膜4と接続する部分また
はその近傍の幅を後部よりも細くするようにしたもので
ある。本実施例によれば、導体部8.5に検出電流11
.12を流したとき、幅の狭くなった導体部では電流密
度が高くなり、磁気抵抗効果膜4の左側ではH工の磁界
が、右側ではH2の磁界が発生する。これにより、磁気
抵抗効果膜4の両端に永久磁石を設けた場合と同様の効
果があり、磁気記録媒体からの信号磁界が入ってきたと
きに、磁気抵抗効果膜の磁区構造のゆらぎを防止するこ
とが可能となって、再生出力波形に生じるバルクハウゼ
ンノイズなどの波形歪をなくすことができるようになる
。(Example 2) FIG. 4 is a perspective view schematically showing the configuration of a magnetoresistive element exemplified in this example. In this example, in the conductor portion 5.8 of the magnetoresistive element 13 shown in Example 1, the width of the portion connected to the magnetoresistive film 4 or its vicinity is narrower than that of the rear part. It is. According to this embodiment, the detection current 11 is applied to the conductor portion 8.5.
.. When a current of 12 is applied, the current density becomes high in the narrow conductor portion, and a magnetic field of H is generated on the left side of the magnetoresistive film 4, and a magnetic field of H2 is generated on the right side of the magnetoresistive film 4. This provides the same effect as when permanent magnets are provided at both ends of the magnetoresistive film 4, and prevents fluctuations in the magnetic domain structure of the magnetoresistive film when a signal magnetic field from a magnetic recording medium enters. This makes it possible to eliminate waveform distortion such as Barkhausen noise that occurs in the reproduced output waveform.
得られた磁気抵抗効果素子について、その特性を調べた
結果、上記実施例1の磁気抵抗効果素子13とほぼ同等
の性能が得られ、動作ならびに効果の点においても全く
同様の結果が得られた。As a result of examining the characteristics of the obtained magnetoresistive element, it was found that almost the same performance as the magnetoresistive element 13 of Example 1 was obtained, and the same results were obtained in terms of operation and effect. .
なお、本実施例においても、バイアス印加手段として導
体膜を磁気抵抗効果膜4の上部に平行に設ける場合を示
したが、その他にシャント膜や電流線あるいは永久磁石
などを用いても本発明の効果は変わらない。また、磁気
シールド用に軟磁性体膜を使用する例を挙げたが、これ
の代わりにバルクの軟磁性体を用いても上記と同様の効
果が得られることは言うまでもない。Although this embodiment also shows the case where a conductive film is provided in parallel above the magnetoresistive film 4 as a bias applying means, the present invention can also be achieved by using a shunt film, a current line, a permanent magnet, etc. The effect remains the same. Further, although an example has been given in which a soft magnetic material film is used for magnetic shielding, it goes without saying that the same effect as described above can be obtained even if a bulk soft magnetic material is used instead.
(実施例 3)
第5図(、)は、本実施例において例示する磁気抵抗効
果素子の構成の概略を示す斜視図で、第5図(b)は第
5図(a)のB−B断面図であって、基板1、絶縁層3
.9、磁気シールド2.10と保護層11により構成さ
れている。本実施例においては、上記実施例1において
示した磁気抵抗効果素子13の磁気抵抗効果膜4の形状
をT字型にしたものである。本実施例によれば、磁気抵
抗効果膜4の先端が飛び出しているため、第5図(b)
に示したように磁気シールド2.10を形成したときに
ギャップ長19を短くすることができる。得られた磁気
抵抗効果素子について、その特性を調べた結果、上記実
施例1の磁気抵抗効果素子13とほぼ同等の性能が得ら
れ、動作ならびに効果の点においても全く同様の結果が
得られた。(Example 3) FIG. 5(,) is a perspective view schematically showing the configuration of the magnetoresistive element illustrated in this example, and FIG. FIG. 2 is a cross-sectional view showing a substrate 1 and an insulating layer 3.
.. 9. Consists of a magnetic shield 2.10 and a protective layer 11. In this embodiment, the shape of the magnetoresistive film 4 of the magnetoresistive element 13 shown in the first embodiment is T-shaped. According to this embodiment, the tip of the magnetoresistive film 4 protrudes, as shown in FIG. 5(b).
The gap length 19 can be shortened when the magnetic shield 2.10 is formed as shown in FIG. As a result of examining the characteristics of the obtained magnetoresistive element, it was found that almost the same performance as the magnetoresistive element 13 of Example 1 was obtained, and the same results were obtained in terms of operation and effect. .
なお、本実施例においても、バイアス印加手段として導
体膜を磁気抵抗効果膜の上部に平行に設置5
ける場合を示したが、その他にシャント膜や電流線ある
いは永久磁石などを用いても本発明の効果は変わらない
。また、磁気シールド用に軟磁性体膜を使用する例を挙
げたが、これの代わりにバルクの軟磁性体を用いても上
記と同様の効果が得られることは言うまでもない。In this embodiment, a conductive film is installed parallel to the upper part of the magnetoresistive film as a bias applying means, but the present invention may also be applied using a shunt film, a current line, a permanent magnet, etc. The effect remains unchanged. Further, although an example has been given in which a soft magnetic material film is used for magnetic shielding, it goes without saying that the same effect as described above can be obtained even if a bulk soft magnetic material is used instead.
(実施例 4)
第6図は、本実施例において例示する磁気抵抗効果素子
の構成の概略を示す斜視図である。本実施例は、上記実
施例1において示した磁気抵抗効果素子13の導体部8
を導体部5と平行に設け、かつ、導体部8の幅はスルー
ホールの幅20よりも広くしたものである。(Example 4) FIG. 6 is a perspective view schematically showing the configuration of a magnetoresistive element exemplified in this example. In this example, the conductor portion 8 of the magnetoresistive element 13 shown in Example 1 above is used.
is provided parallel to the conductor portion 5, and the width of the conductor portion 8 is wider than the width 20 of the through hole.
本実施例では、まず、導体部8から導体部5に向かって
検出電流iを流す。導体部8の幅は、スルーホールの幅
20に比べて広いため、検出電流iは導体部8の幅方向
からスルーホール中心へ向かって、ちょうど磁気抵抗効
果膜4に平行となるように流れる。これにより、上記実
施例1のように導体部8を磁気抵抗効果膜4と平行に設
けた場合と同様、導体部8がバイアス印加手段ともなり
得る。In this embodiment, first, a detection current i is caused to flow from the conductor section 8 toward the conductor section 5. Since the width of the conductor portion 8 is wider than the width 20 of the through hole, the detection current i flows from the width direction of the conductor portion 8 toward the center of the through hole so as to be exactly parallel to the magnetoresistive film 4 . Thereby, the conductor part 8 can also serve as a bias applying means, similar to the case where the conductor part 8 is provided in parallel with the magnetoresistive film 4 as in the first embodiment.
得られた磁気抵抗効果素子について、その特性を調べた
結果、上記実施例1の磁気抵抗効果素子13とほぼ同等
の性能が得られ、動作ならびに効果の点においても全く
同様の結果が得られた。As a result of examining the characteristics of the obtained magnetoresistive element, it was found that almost the same performance as the magnetoresistive element 13 of Example 1 was obtained, and the same results were obtained in terms of operation and effect. .
なお、本実施例においても、磁気抵抗効果膜の上部にシ
ャント膜や電流線あるいは永久磁石などを用いても本発
明の効果は変わらない。また、磁気シールド用に軟磁性
体膜を使用する例を挙げたが、これの代わりにバルクの
軟磁性体を用いても上記と同様の効果が得られることは
言うまでもない。In this embodiment, even if a shunt film, a current line, a permanent magnet, or the like is used above the magnetoresistive film, the effects of the present invention do not change. Further, although an example has been given in which a soft magnetic material film is used for magnetic shielding, it goes without saying that the same effect as described above can be obtained even if a bulk soft magnetic material is used instead.
以上詳細に説明したごとく、本発明の磁気抵抗効果素子
は、磁気抵抗効果膜の中央部膜面上に1本と両端に2本
の導体部を設けることで、従来の差動型の磁気抵抗効果
素子と同様の効果が得られるので、狭トラック化に対応
して高密度記録再生を実現できると同時に、狭トラック
化してもダイナミックレンジの拡大および低雑音化を達
成できる効果がある。As explained in detail above, the magnetoresistive element of the present invention has one conductor section on the central film surface of the magnetoresistive film and two conductor sections at both ends, so that the magnetoresistive element of the present invention is different from the conventional differential type magnetoresistive element. Since the same effect as an effect element can be obtained, it is possible to realize high-density recording and reproduction in response to narrower tracks, and at the same time, it is possible to achieve the effect of expanding the dynamic range and reducing noise even with narrower tracks.
第1図は本発明の実施例1において例示した磁気抵抗効
果素子の構成の概略を示す斜視図、第2図(a)は第1
図の構成を示す平面図、第2図(b)は第2図(、)の
A−A断面図、第3図は実施例1に示した磁気抵抗効果
素子の動作を示す説明図、第4図は本発明の実施例2に
おいて例示した磁気抵抗効果素子の構成の概略を示す斜
視図、第5図(a)は本発明の実施例3において例示し
た磁気抵抗効果素子の構成の概略を示す斜視図、第5図
(b)は第5図(a)のB−B断面図、第6図は本発明
の実施例4において例示した磁気抵抗効果素子の構成の
概略を示す斜視図である。
1・・・基板 2.10・・・磁気シール
ド3.6.9・・・絶縁層 4・・・磁気抵抗効果膜
5.8・・・導体部 7・・・スルーホール11
・・・保護層 12・・・パッド部13・・・
磁気抵抗効果素子
4・・・磁気記録媒体 15・・・磁界信号6・・・
正側に変化した電圧変化
7・・・負側に変化した電圧変化FIG. 1 is a perspective view schematically showing the structure of the magnetoresistive element illustrated in Example 1 of the present invention, and FIG.
2(b) is a sectional view taken along the line A-A in FIG. 2(a); FIG. FIG. 4 is a perspective view schematically showing the structure of the magnetoresistive element illustrated in Example 2 of the present invention, and FIG. 5(a) is a perspective view schematically showing the structure of the magnetoresistive element illustrated in Example 3 of the present invention. FIG. 5(b) is a sectional view taken along line BB in FIG. 5(a), and FIG. 6 is a perspective view schematically showing the structure of the magnetoresistive element illustrated in Example 4 of the present invention. be. 1... Substrate 2.10... Magnetic shield 3.6.9... Insulating layer 4... Magnetoresistive film 5.8... Conductor part 7... Through hole 11
...Protective layer 12...Pad portion 13...
Magnetoresistive element 4...Magnetic recording medium 15...Magnetic field signal 6...
Voltage change that changed to the positive side 7... Voltage change that changed to the negative side
Claims (1)
抗効果膜と、該磁気抵抗効果膜にバイアスを印加する手
段と、上記磁気抵抗効果膜に電流を流すと同時に、その
電圧を読取る導体部を、上記磁気抵抗効果膜の両端部と
中央部の3箇所に設け、さらに上記磁気抵抗効果膜を磁
気的にシールドする一対の磁気シールド部材よりなる磁
気抵抗効果素子であって、少なくとも上記磁気抵抗効果
膜上では、上記中央部の導体部により形成される電極部
を、磁気記録媒体のトラック幅方向にほぼ平行に構成し
たことを特徴とする磁気抵抗効果素子。 2、請求の範囲第1項において、磁気抵抗効果膜の中央
部に接続した導体部に流れる信号検出電流の方向が、少
なくとも磁気抵抗効果膜上では、磁気記録媒体のトラッ
ク幅方向にほぼ平行となるように構成したことを特徴と
する磁気抵抗効果素子。 3、請求の範囲第1項または第2項において、中央部に
設けた導体部と磁気抵抗効果膜の接続部の幅とトラック
幅の比を1/2〜1/40としたことを特徴とする磁気
抵抗効果素子。 4、請求の範囲第1項、第2項または第3項記載の磁気
抵抗効果素子の磁気抵抗効果膜の両端部に接続する2本
の導体部において、磁気抵抗効果膜と接続する部分また
はその近傍の導体部の幅を、該導体部の後部の幅よりも
小さくしたことを特徴とする磁気抵抗効果素子。 5、請求の範囲第1項ないし第4項のいずれか1項記載
の磁気抵抗効果素子において、磁気抵抗効果膜の形状を
T字型としたことを特徴とする磁気抵抗効果素子。 6、請求の範囲第1項ないし第5項のいずれか1項記載
の磁気抵抗効果素子において、磁気抵抗効果膜の両側に
薄膜もしくはバルクの磁気シールド部材を設けたことを
特徴とする磁気抵抗効果素子。 7、請求の範囲第1項ないし第6項のいずれか1項記載
の磁気抵抗効果素子において、バイアス印加手段として
、シャント膜、電流線、永久磁石のうちから選ばれる少
なくとも1つ以上を組合せて用いて構成したことを特徴
とする磁気抵抗効果素子。 8、請求の範囲第1項ないし第7項のいずれか1項記載
の磁気抵抗効果素子において、導体部を磁気抵抗効果膜
の上部もしくは下部に設けたことを特徴とする磁気抵抗
効果素子。9、請求の範囲第1項ないし第8項のいずれ
か1項記載の磁気抵抗効果素子を用いて、狭トラック化
された高密度磁気記録媒体からの漏洩磁束信号を、高感
度に検出して記録情報を読取る磁気ヘッドを構成したこ
とを特徴とする磁気ヘッド。 10、請求の範囲第9項記載の磁気ヘッドを用いて、高
密度磁気記録媒体からの漏洩磁束信号を検出して、上記
磁気記録媒体に記録されている情報の読取りを行う手段
を設けたことを特徴とする磁気記録再生装置。[Scope of Claims] 1. A magnetoresistive film for detecting a leakage magnetic flux signal from a magnetic recording medium, means for applying a bias to the magnetoresistive film, and simultaneously applying a current to the magnetoresistive film, The magnetoresistive element comprises conductor parts for reading the voltage, which are provided at three locations at both ends and the center of the magnetoresistive film, and a pair of magnetic shield members that magnetically shield the magnetoresistive film. A magnetoresistive element characterized in that, at least on the magnetoresistive film, an electrode portion formed by the central conductor portion is arranged substantially parallel to the track width direction of the magnetic recording medium. 2. In claim 1, the direction of the signal detection current flowing through the conductor connected to the center of the magnetoresistive film is substantially parallel to the track width direction of the magnetic recording medium, at least on the magnetoresistive film. A magnetoresistive effect element characterized by being configured so that: 3. Claim 1 or 2 is characterized in that the ratio of the width of the connection portion between the conductor portion provided in the center and the magnetoresistive film to the track width is 1/2 to 1/40. A magnetoresistance effect element. 4. In the two conductor portions connected to both ends of the magnetoresistive film of the magnetoresistive element according to claim 1, 2, or 3, the portion connected to the magnetoresistive film or its A magnetoresistive element characterized in that the width of a nearby conductor part is smaller than the width of the rear part of the conductor part. 5. A magnetoresistive element according to any one of claims 1 to 4, characterized in that the magnetoresistive film has a T-shape. 6. The magnetoresistive element according to any one of claims 1 to 5, characterized in that a thin film or bulk magnetic shielding member is provided on both sides of the magnetoresistive film. element. 7. In the magnetoresistive element according to any one of claims 1 to 6, the bias applying means is a combination of at least one selected from a shunt film, a current line, and a permanent magnet. 1. A magnetoresistive effect element configured using 8. A magnetoresistive element according to any one of claims 1 to 7, characterized in that a conductor portion is provided above or below the magnetoresistive film. 9. A leakage magnetic flux signal from a narrow track high-density magnetic recording medium is detected with high sensitivity using the magnetoresistive element according to any one of claims 1 to 8. A magnetic head comprising a magnetic head for reading recorded information. 10. A means for reading information recorded on the magnetic recording medium by detecting leakage magnetic flux signals from the high-density magnetic recording medium using the magnetic head according to claim 9 is provided. A magnetic recording/reproducing device characterized by:
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP14126590A JPH0438614A (en) | 1990-06-01 | 1990-06-01 | Magneto-resistance effect element and its applied magnetic head and recording and reproducing device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP14126590A JPH0438614A (en) | 1990-06-01 | 1990-06-01 | Magneto-resistance effect element and its applied magnetic head and recording and reproducing device |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0438614A true JPH0438614A (en) | 1992-02-07 |
Family
ID=15287881
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP14126590A Pending JPH0438614A (en) | 1990-06-01 | 1990-06-01 | Magneto-resistance effect element and its applied magnetic head and recording and reproducing device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0438614A (en) |
-
1990
- 1990-06-01 JP JP14126590A patent/JPH0438614A/en active Pending
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US5218497A (en) | Magnetic recording-reproducing apparatus and magnetoresistive head having two or more magnetoresistive films for use therewith | |
| US5193038A (en) | Shorted dual element magnetoresistive reproduce head exhibiting high density signal amplification | |
| US5592082A (en) | Magnetic sensor with permanent magnet bias layers | |
| JPH0473201B2 (en) | ||
| US5535077A (en) | Magnetoresistive head having magnetically balanced magnetoresistive elements laminated on opposite sides of an electrically conductive film | |
| JPH07176019A (en) | Flat magnetoresistance head | |
| KR100267411B1 (en) | Magnetoresistive head | |
| EP0372420B1 (en) | Magnetic recording-reproducing apparatus and magnetoresistive head for use therewith | |
| JP2662334B2 (en) | Thin film magnetic head | |
| EP0514976A2 (en) | Combined read/write magnetic head | |
| JP3394549B2 (en) | Horizontal magnetoresistive thin film magnetic head | |
| JP2583851B2 (en) | Magnetoresistive magnetic head | |
| JPH08203032A (en) | Magnetoresistive effect reproducing head | |
| JPH0441415B2 (en) | ||
| JPS6134577Y2 (en) | ||
| JP3040892B2 (en) | Magnetoresistive thin film magnetic head | |
| JP3175176B2 (en) | Magnetoresistive head | |
| JPH05266437A (en) | Magnetoresistive head | |
| JPH07153023A (en) | Magnetic thin-film head for read and write | |
| JPH07110921A (en) | Magnetoresistance effect type thin film head | |
| JPH0546946A (en) | Magnetoresistance effect type head | |
| JPH02130712A (en) | magnetoresistive element | |
| JPH0378106A (en) | Magnetoresistive element and magnetic recording/reproducing device using the same | |
| JPH05182146A (en) | Thin film magnetic head | |
| JPH05159247A (en) | Magneto-resistance effect head |