JPH04205903A - Method and device for reproducing signal by magnetoresistance effect type head and recording device using the same - Google Patents

Method and device for reproducing signal by magnetoresistance effect type head and recording device using the same

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Publication number
JPH04205903A
JPH04205903A JP33019390A JP33019390A JPH04205903A JP H04205903 A JPH04205903 A JP H04205903A JP 33019390 A JP33019390 A JP 33019390A JP 33019390 A JP33019390 A JP 33019390A JP H04205903 A JPH04205903 A JP H04205903A
Authority
JP
Japan
Prior art keywords
signal
reproducing device
asymmetry
magnetic field
magnetoresistive
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
JP33019390A
Other languages
Japanese (ja)
Inventor
Isamu Yuhito
勇 由比藤
Masahiro Kitada
北田 正弘
Naoki Koyama
直樹 小山
Yasuhiro Kato
泰裕 加藤
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 JP33019390A priority Critical patent/JPH04205903A/en
Publication of JPH04205903A publication Critical patent/JPH04205903A/en
Pending legal-status Critical Current

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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
    • G11B5/02Recording, reproducing, or erasing methods; Read, write or erase circuits therefor
    • G11B5/027Analogue recording
    • G11B5/035Equalising

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  • Magnetic Heads (AREA)
  • Recording Or Reproducing By Magnetic Means (AREA)

Abstract

PURPOSE:To reduce asymmetry in a regenerative signal waveform and fluctuation of an output due to variations of head characteristics by providing a means for optimizing the magnetizing direction of a magnetoresistance effect film in changing the intensity of a bias magnetic field to be impressed upon the magnetoresistance effect film. CONSTITUTION:The subject device is provided with the means for optimizing the magnetizing direction of the magnetoresistance effect film in changing the intensity of the bias magnetic field to be impressed upon the magnetoresistance effect film. For example, a waveform reproduced by a magnetoresistance effect type head 2 is detected by a waveform asymmetry degree detecting part 4 in an unbalanced ant. between the plus side and minus side of the regenerative signal, and the unbalanced amt. and a reference symmetry degree signal are compared with each other by a comparing part 5 to detect their difference. An output of the comparing part 5 is given to a sense power source 6 for deciding a conductive current value to the magnetoresistance effect film, and a sense current value is varied according to the size of the output of the comparing part 5. By this method, the bias magnetic field is optimized, and asymmetry of the regenerative signal waveform and fluctuation of the reproducing output can be prevented.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、磁気ディスク装置あるいはVTR等の磁気テ
ープ装置に好適に用いられる再生専用の磁気抵抗効果型
ヘッドによる信号再生方法と装置およびそれを用いた記
録装置に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a signal reproducing method and apparatus using a magnetoresistive head exclusively used for reproduction, which is suitably used in a magnetic disk device or a magnetic tape device such as a VTR. Regarding the recording device used.

〔従来の技術〕[Conventional technology]

最近の磁気記録装置の記憶容量の増大に伴い。 With the increase in storage capacity of recent magnetic recording devices.

例えば磁気ディスク装置ではトラック幅は数μm程度に
なりつつある。また、記録装置は小型化され、低周速度
になっている。このように狭く記録された信号を高S(
シグナル)/N(ノイズ)に検出する磁気ヘッドとして
、従来の誘導型ヘッドに代わり磁気抵抗効果型ヘッドの
開発が進められている。例えば、第13回日本応用磁気
学会学術講演概要集(1989年)第228頁。
For example, in magnetic disk drives, the track width is becoming approximately several μm. In addition, recording devices have become smaller and have lower peripheral speeds. In this way, the narrowly recorded signal is converted into a high S (
As a magnetic head for detecting signal)/N (noise), a magnetoresistive head is being developed in place of the conventional inductive head. For example, the 13th Japanese Society of Applied Magnetics Academic Lecture Abstracts (1989), p. 228.

磁気抵抗効果型ヘッドは2例えば第5図に示したような
構造をしている。図に示す磁気抵抗効果型ヘッドは、シ
ャントバイアス型ヘッドと呼ばれているものである。磁
気抵抗効果型ヘッドは、基板の上部と下部に積層された
シールド膜21.磁気抵抗効果[I!19.シャントバ
イアス膜20および電極18等により構成されている。
A magnetoresistive head has a structure as shown in FIG. 5, for example. The magnetoresistive head shown in the figure is called a shunt bias type head. The magnetoresistive head has a shield film 21 laminated on the upper and lower parts of the substrate. Magnetoresistive effect [I! 19. It is composed of a shunt bias film 20, an electrode 18, and the like.

磁気抵抗効果型ヘッドにおいて、再生出力を高め、かつ
信号波形の非対称性を低減するために。
To increase reproduction output and reduce signal waveform asymmetry in magnetoresistive heads.

磁気抵抗効果膜19にバイアス磁界を印加しなければな
らない。これを、第6図を用いて説明する。
A bias magnetic field must be applied to the magnetoresistive film 19. This will be explained using FIG. 6.

第6図は、磁気抵抗効果膜19の出力−磁界曲線である
。磁気抵抗効果型ヘッドは、出力−磁界曲線の最も急峻
で直線性の良い領域を用いて、信号磁界22に対する再
生出力23を得る。このために、一定のバイアス磁界H
bを印加して用いられる。上記のシャントバイアス型ヘ
ッドでは、シャントバイアス1I20に流れる電流によ
り発生する磁界でバイアス磁界Hbを印加する。
FIG. 6 is an output-magnetic field curve of the magnetoresistive film 19. The magnetoresistive head obtains a reproduction output 23 for a signal magnetic field 22 by using the steepest and most linear region of the output-magnetic field curve. For this purpose, a constant bias magnetic field H
It is used by applying b. In the shunt bias type head described above, a bias magnetic field Hb is applied by a magnetic field generated by a current flowing through the shunt bias 1I20.

しかし9例えばシャントバイアス型ヘッドではシャント
バイアス膜20の膜厚、あるいは比抵抗の変動によりシ
ャント電流値が変化しやすく、バイアス磁界Hbも変動
してしまう。これは、他のバイアス方式のヘッドでも同
様である。このために、1〜ラック幅の大きな磁気抵抗
効果型ヘッドでは、従来は差動型のヘッド構造がとられ
ていた。
However, in a shunt bias type head, for example, the shunt current value tends to change due to changes in the film thickness or specific resistance of the shunt bias film 20, and the bias magnetic field Hb also changes. This also applies to heads using other bias methods. For this reason, magnetoresistive heads with large rack widths have conventionally adopted a differential head structure.

第7図に差動型磁気抵抗効果型ヘッドの概略を示す。こ
の方式の1つは、1トラツクを2つに分けた3つの端子
24.25.26を持つ構造のヘッドである。端子25
を共通として端子24.26から電流を流す。これによ
り、それぞれの端子間の磁気抵抗効果膜19には、矢印
で示す互いに逆方向のバイアス磁界を印加できる。信号
磁界は。
FIG. 7 schematically shows a differential magnetoresistive head. One of these systems is a head having three terminals 24, 25, and 26 that divide one track into two. terminal 25
A current is passed from terminals 24 and 26 with the terminals being common. Thereby, bias magnetic fields in mutually opposite directions indicated by arrows can be applied to the magnetoresistive film 19 between the respective terminals. The signal magnetic field is.

共に同方向に印加される。このために9両端子間での信
号は逆位相となり、端子間の信号E□、E2の差を検出
することにより信号波形の非対称性が改善できる。とこ
ろが、記録密度が高まり狭トラツク化がすすむにつれて
、上記差動型磁気抵抗効果型ヘッドでは、その構造上狭
トラツク化したヘッドを構成することが困難であり、そ
のため新たな信号処理方式が望まれていた。
Both are applied in the same direction. Therefore, the signals between the nine terminals have opposite phases, and by detecting the difference between the signals E□ and E2 between the terminals, the asymmetry of the signal waveform can be improved. However, as recording density increases and tracks become narrower, it is difficult to construct a head with narrower tracks due to the structure of the differential magnetoresistive head described above, and a new signal processing method is therefore desired. was.

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

上述したように、差動型磁気抵抗効果型ヘッドは、その
構造上狭トラツク化したヘッドの構成が困難であり、ま
た差動型以外の従来の磁気抵抗効果型ヘッドにおいては
、バイアス磁界の適正化についての考慮は全くされてい
なかった。このために、再生信号波形が非対称性となり
、再生信号にピークシフトなどが生じる等、信号再生時
にエラーとなりやすかった。また、再生出力も変動しや
すい等の問題もあった。
As mentioned above, it is difficult to construct a narrow track head with a differential magnetoresistive head due to its structure, and in conventional magnetoresistive heads other than the differential type, it is difficult to set the bias magnetic field appropriately. No consideration was given to conversion. For this reason, the reproduced signal waveform becomes asymmetrical, and errors such as peak shifts occur in the reproduced signal, which tend to occur during signal reproduction. Further, there were also problems such as the playback output being easily fluctuated.

厳密に管理されたヘッド作製工程を構築することも考え
られるが、その工程には避けがたい磁気抵抗効果膜の膜
厚や比抵抗の変動があり、実際に。
Although it is conceivable to establish a strictly controlled head manufacturing process, there are unavoidable variations in the film thickness and resistivity of the magnetoresistive film in that process, and in practice.

ヘッド作製工程を厳密に管理することは極めて困難であ
り、製品の歩留まりの低下、あるいはコストの上昇を生
じてしまうという問題があった。
It is extremely difficult to strictly control the head manufacturing process, resulting in a problem of a decrease in product yield or an increase in cost.

本発明の目的は、上記従来技術における問題点である磁
気抵抗効果型ヘッドの再生信号波形の非対称性、再生信
号に生じるピークシフトおよび再生出力の変動等を好適
に抑制することが可能な信号再生方法とその装置および
それを用いた情報の記録装置を提供することにある。
An object of the present invention is to provide a signal reproducing system capable of suitably suppressing problems in the prior art described above, such as asymmetry of the reproduced signal waveform of the magnetoresistive head, peak shifts occurring in the reproduced signal, and fluctuations in the reproduced output. The object of the present invention is to provide a method, a device thereof, and an information recording device using the same.

〔課題を解決するための手段〕[Means to solve the problem]

上記本発明の課題を解決するために、磁気抵抗効果型ヘ
ッドの磁気抵抗効果膜に印加するバイアス磁界の強度を
変えて磁気抵抗効果膜の磁化方向が最適化されるように
、磁気抵抗効果膜への通電電流値を可変可能に構成し、
バイアス磁界の適正化をはかるものである。
In order to solve the above-mentioned problems of the present invention, the magnetoresistive film is designed such that the magnetization direction of the magnetoresistive film is optimized by changing the intensity of the bias magnetic field applied to the magnetoresistive film of the magnetoresistive head. The energizing current value is configured to be variable,
This aims to optimize the bias magnetic field.

すなわち、シャントバイアス型ヘッドにおいて。That is, in a shunt bias type head.

磁気抵抗効果膜への通電電流(センス電流)値を変える
ことは、シャントバイアス膜の電流値も同時に変わるこ
とであり、バイアス磁界を可変とすることができ、その
適正化をはかることが可能となる。また、ソフトバイア
ス型ヘッドでは、上記と同様に磁気抵抗効果膜へのセン
ス電流値を変えることにより、ソフトバイアス膜の磁化
状態が変わりバイアス磁界の適正化をはかることができ
る。
Changing the value of the current flowing to the magnetoresistive film (sense current) also changes the current value of the shunt bias film at the same time, making it possible to vary the bias magnetic field and optimize it. Become. Further, in a soft bias type head, by changing the sense current value to the magnetoresistive film as described above, the magnetization state of the soft bias film changes and the bias magnetic field can be optimized.

本発明は、磁気抵抗効果型ヘッドを用いて記録媒体に記
録されている情報を再生する信号再生装置において、磁
気抵抗効果膜に印加されるバイアス磁界の強度を変えて
磁気抵抗効果膜の磁化方向を最適化する手段を設けるも
のであって2例えば磁気抵抗効果型ヘッドの再生信号波
形の非対称度を検出する手段と、上記信号波形の非対称
度に対応して磁気抵抗効果膜への通電電流値を変えるこ
とにより、バイアス磁界の強度を変えて磁気抵抗効果膜
の磁化方向を最適化する手段を有するものである。そし
て、上記信号波形の非対称度を検出する手段は、信号波
形のプラス側ピーク値とマイナス側ピーク値との差を検
出する手段等を用いることができる。
The present invention provides a signal reproducing device that reproduces information recorded on a recording medium using a magnetoresistive head, in which the direction of magnetization of the magnetoresistive film is changed by changing the intensity of a bias magnetic field applied to the magnetoresistive film. 2. For example, a means for detecting the degree of asymmetry of the reproduced signal waveform of a magnetoresistive head, and a means for optimizing the current flowing through the magnetoresistive film in accordance with the degree of asymmetry of the signal waveform. The present invention has means for optimizing the magnetization direction of the magnetoresistive film by changing the strength of the bias magnetic field. The means for detecting the degree of asymmetry of the signal waveform may be a means for detecting a difference between a positive peak value and a negative peak value of the signal waveform.

また2本発明の磁気抵抗効果型ヘッドを用いた信号再生
装置において、磁気抵抗効果膜への通電電流値情報を、
読み出し専用の半導体メモリに記憶させておき、上記通
電電流値情報をもとにバイアス磁界の強度を変えて磁気
抵抗効果膜の磁化方向を最適化することもできる。
In addition, in the signal reproducing device using the magnetoresistive head of the present invention, information on the value of current flowing to the magnetoresistive film is
It is also possible to store the information in a read-only semiconductor memory and to optimize the magnetization direction of the magnetoresistive film by changing the strength of the bias magnetic field based on the information on the current value.

本発明の磁気抵抗効果型ヘッドを用いた信号再生装置に
おいて、該信号再生装置の使用前に少なくとも1度、磁
気抵抗効果膜への通電電流値を最適化するように動作さ
せるものであり9例えば記録媒体に1,0の信号を記録
させ、該信号で信号波形のプラス側ピーク値とマイナス
側ピーク値との差を検出し、磁気抵抗効果膜への通電電
流値を制御しバイアス磁界の最適化をはかることができ
る。そして、バイアス磁界の強度を変えて磁気抵抗効果
膜の磁化方向を最適化するための信号は。
In the signal reproducing device using the magnetoresistive head of the present invention, the signal reproducing device is operated at least once to optimize the value of current flowing through the magnetoresistive film before use. A signal of 1 or 0 is recorded on the recording medium, and the difference between the positive peak value and the negative peak value of the signal waveform is detected using the signal, and the current value applied to the magnetoresistive film is controlled to optimize the bias magnetic field. It is possible to make changes. And the signal for optimizing the magnetization direction of the magnetoresistive film by changing the strength of the bias magnetic field.

常に記録媒体に保存されているか、または情報を再生す
るために記録されている記録媒体の必要不可欠なデータ
からの信号とするものである。
It is a signal from essential data of a recording medium that is always stored on the recording medium or recorded for reproducing information.

さらに9本発明の磁気抵抗効果型ヘッドを用いた信号再
生装置と情報の記録装置とを組み合わせて、情報の記録
および再生を行う記録再生装置を構成することができる
Further, by combining a signal reproducing device using the magnetoresistive head of the present invention and an information recording device, a recording/reproducing device for recording and reproducing information can be constructed.

〔作用〕[Effect]

以下2本発明の作用を第1図を用いて説明する。 The following two effects of the present invention will be explained using FIG.

図において、記録媒体1に記録された信号を、磁気抵抗
効果型ヘッド2で再生する。再生信号は一般に微弱であ
り、必要に応じアンプ3で増幅する。
In the figure, a signal recorded on a recording medium 1 is reproduced by a magnetoresistive head 2. The reproduced signal is generally weak and is amplified by the amplifier 3 if necessary.

アンプ3からの出力は、波形非対称度検出部4に入る。The output from the amplifier 3 enters a waveform asymmetry detection section 4.

ここでは、再生信号のプラス側とマイナス側のアンバラ
ンス量を検出する。比較部5で、上記アンバランス量と
基準対称度信号とを比較し。
Here, the amount of imbalance between the plus side and the minus side of the reproduced signal is detected. A comparison section 5 compares the unbalance amount with the reference symmetry degree signal.

その差分を検出する。基準対称度信号とは、装置駆動上
許される非対称度しこ対応する信号で、上記基準対称度
信号以下であれば装置は正常に動作する。比較部5の出
力は、磁気抵抗効果膜19(第5図参照)への通電電流
値を決定するセンス電源6に与えられ、比較部5の出力
の大小によりセンス電流値が可変される。以上の動作に
より、ノスイアス磁界Hbを適正化でき、再生信号波形
の非対称性および再生出力の変動を防止することができ
る。なお、上記一連の動作は実際の記録信号を再生する
前に行う必要がある。
Detect the difference. The reference symmetry degree signal is a signal corresponding to the degree of asymmetry allowed for driving the device, and the device operates normally if the degree of asymmetry is equal to or less than the reference symmetry degree signal. The output of the comparator 5 is applied to a sense power supply 6 that determines the value of the current flowing to the magnetoresistive film 19 (see FIG. 5), and the sense current value is varied depending on the magnitude of the output of the comparator 5. By the above operation, the noisy magnetic field Hb can be optimized, and asymmetry in the reproduced signal waveform and fluctuation in the reproduced output can be prevented. Note that the above series of operations must be performed before actually reproducing the recorded signal.

〔実施例〕〔Example〕

以下に本発明の実施例を挙げ7図面を引用してさらに詳
細に説明する。
Embodiments of the present invention will be described in more detail below with reference to seven drawings.

(実施例1) 第1図を用いて説明する。用いた磁気抵抗効果型ヘッド
2はシャントバイアス型ヘッドで、トラック幅は5μm
である。第5図に示すごとく、磁気抵抗効果膜19.お
よびシャントバイアス膜20のセンス電流値は、共に1
0mAとした。初めに、記録媒体1.0の連続した信号
を誘導型薄膜ヘッドで記録した。次に、上記磁気抵抗効
果型ヘッドで上記信号の再生を行った。このような動作
は、信号再生装置内に記憶させておいたソフトで自動的
に行った。この磁気抵抗効果型ヘッドの上記センス電流
値における再生波形の非対称度は30%であった。なお
、再生波形の非対称度とは。
(Example 1) This will be explained using FIG. 1. The magnetoresistive head 2 used was a shunt bias type head, and the track width was 5 μm.
It is. As shown in FIG. 5, the magnetoresistive film 19. and the sense current value of the shunt bias film 20 are both 1
It was set to 0mA. First, continuous signals on recording medium 1.0 were recorded with an inductive thin film head. Next, the signal was reproduced using the magnetoresistive head. Such operations were automatically performed using software stored in the signal reproducing device. The degree of asymmetry of the reproduced waveform of this magnetoresistive head at the above sense current value was 30%. Furthermore, what is the degree of asymmetry of the reproduced waveform?

再生信号のプラス側ピーク値IP、マイナス側ピーク値
工、とじて。
The plus side peak value IP, the minus side peak value, and the end of the reproduced signal.

再生波形の非対称度(%)=(Ip  I−)/(Ip
+I−)X100で表わされる。ここで用いたヘッドの
再生出力値は、単位トラック幅当り7oμVp−p/μ
mであった。したがってt Ip=45.5μV、 ■
、=24.5μVである。再生信号が非常に微弱である
ために、アンプ3で100倍の増幅を行った。
Asymmetry of reproduced waveform (%) = (Ip I-)/(Ip
+I−)X100. The playback output value of the head used here is 7oμVp-p/μ per unit track width.
It was m. Therefore, tIp=45.5μV, ■
, =24.5 μV. Since the reproduced signal was very weak, amplifier 3 amplified it 100 times.

次に、波形非対称度検出部4で再生信号波形の非対称度
を検出した。波形非対称度の検出は、第2図に示すピー
ク値検出法を用いた。このピーク値検出法は、プラスピ
ークホールド部7.マイナスピークホールド部8.およ
び差動増幅部9より構成した。すなわち、再生信号波形
のプラス側ピーク値IPをプラスピークホールド部7で
、また。
Next, the waveform asymmetry detecting section 4 detected the asymmetry of the reproduced signal waveform. The peak value detection method shown in FIG. 2 was used to detect the degree of waveform asymmetry. This peak value detection method uses the plus peak hold section 7. Minus peak hold section 8. and a differential amplifier section 9. That is, the plus side peak value IP of the reproduced signal waveform is held by the plus peak hold section 7.

マイナス側ピーク値■1とマイナスピークホールド部8
で検出する。Ipおよび■1は、差動増幅部9でそのア
ンバランス量を検出する。差動増幅部9の増幅度は10
倍とした。これにより、差動増幅部9の出力として21
mVを得た。基準非対称度信号■、としては、波形非対
称度5%に相当する3、5mVを与えた。この結果、比
較部5がらの両信号の差17.5mVがセンス電源部6
ヘフイードバツクされ、センス電流値が小さくなる方向
に調整された。
Negative peak value ■1 and negative peak hold part 8
Detect with. The unbalance amount of Ip and (1) is detected by the differential amplifier section 9. The amplification degree of the differential amplifier section 9 is 10
It was doubled. As a result, the output of the differential amplifier section 9 is 21
mV was obtained. As the reference asymmetry signal (■), 3.5 mV, which corresponds to a waveform asymmetry of 5%, was given. As a result, the difference of 17.5 mV between both signals from the comparator 5 is the sense power supply 6.
Feedback was performed and the sense current value was adjusted to become smaller.

波形非対称度を測定するために2本実施例では1.0の
信号をあらかじめ記録したが、記録媒体に記録されるア
ドレス情報、同期情報などの信号再生に必要不可欠な信
号を用いることも可能である。
In order to measure the degree of waveform asymmetry, a signal of 1.0 was recorded in advance in this example, but it is also possible to use signals essential for signal reproduction such as address information and synchronization information recorded on the recording medium. be.

(実施例2) 上記実施例1は、実時間でセンス電流値を制御するタイ
プであるが、トランク幅がより狭くなり再生信号が微弱
になると9回路系の持つノイズにより正確なセンス電流
の制御が困難となる。本実施例においては、ノイズの影
響を低減しより正確にセンス電流の制御を行うようにし
たものであり。
(Example 2) The above-mentioned Example 1 is a type that controls the sense current value in real time, but as the trunk width becomes narrower and the reproduction signal becomes weaker, the sense current is controlled more accurately due to the noise of the 9-circuit system. becomes difficult. In this embodiment, the influence of noise is reduced and the sense current is controlled more accurately.

第3図を用いて説明する。本実施例では、波形非対称度
検出部4をプラス側ピーク値検出部10゜マイナス側ピ
ーク値検出部13.平均値演算部11.12.および差
動増幅部9により構成した。
This will be explained using FIG. In this embodiment, the waveform asymmetry detecting section 4 is divided into a plus side peak value detecting section 10°, a minus side peak value detecting section 13. Average value calculation unit 11.12. and a differential amplifier section 9.

特に、平均値演算部11.12を設けたことが実施例1
とは異なる。この構成により、ある一定時間内の複数の
ピーク値を検出し、かつその平均的ピーク値を求めた。
In particular, the provision of the average value calculation units 11 and 12 is the first embodiment.
It is different from. With this configuration, a plurality of peak values within a certain period of time were detected, and the average peak value was determined.

本実施例では1000個のピーク値の平均を求めた。そ
の結果、トラック@1μmのヘッドにおいてもセンス電
流値を十分に制御することができた。なお2本実施例に
おいてはシャントバイアス型ヘッドを用いたが、ソフト
バイアス型ヘッドにおいても上記と同様の効果が得られ
た。
In this example, the average of 1000 peak values was calculated. As a result, it was possible to sufficiently control the sense current value even in a head with a track of 1 μm. Although a shunt bias type head was used in the second embodiment, the same effect as described above was obtained with a soft bias type head.

(実施例3) 上記実施例1および2はセンス電流値がメモリに保存さ
れていない場合の例である。このために。
(Third Embodiment) The first and second embodiments described above are examples in which the sense current value is not stored in the memory. For this.

ヘッドの非動作時間には、センス電流を下げておくよう
な使い方をする場合には、センス電流の制御をやりなお
さなくてはならない。このことは。
If the sense current is to be lowered during head non-operation time, the sense current must be controlled again. About this.

高速性を要求されている磁気記録装置においては時間の
損失となり好ましくない。本実施例は、上記の問題点に
対処するものであり、第4図を用いて説明する。図に示
すごとく、比較部5の出力をA(アナログ)/D(ディ
ジタル)コンバータ14を介しディジタル化し、さらに
メモリ15内に記憶するようにした。さらに、メモリの
記憶された信号をD/Aコンバータ16で再度アナログ
信号に変換し、センス電源6に与えるようにした。
In a magnetic recording device that requires high speed, this is undesirable as it results in a loss of time. This embodiment deals with the above problem and will be explained using FIG. 4. As shown in the figure, the output of the comparator 5 is digitized via an A (analog)/D (digital) converter 14 and further stored in a memory 15. Furthermore, the signal stored in the memory is converted again into an analog signal by the D/A converter 16, and is applied to the sense power supply 6.

これにより、センス電流は常にメモリ15に保存されて
おり、上記の問題に対処できる。また、メモリ15をバ
ッテリバックアップしておくことにより、停電時にも対
処でき、装置の再起動の時間を短縮することができた。
Thereby, the sense current is always stored in the memory 15, and the above problem can be solved. Furthermore, by backing up the memory 15 with a battery, it is possible to cope with a power outage, and the time required to restart the apparatus can be shortened.

また、磁気抵抗効果型ヘッドを、信号再生装置に搭載前
に最適センス電流値を測定しておき、かつ上記最適セン
ス電流値情報を、読み出し専用半導体メモリに記憶して
おくことも有効である。この場合には、信号再生装置側
には非対称度検出系。
It is also effective to measure the optimum sense current value before installing the magnetoresistive head in the signal reproducing device, and to store the optimum sense current value information in a read-only semiconductor memory. In this case, an asymmetry detection system is provided on the signal reproducing device side.

さらには電流値の制御系が不用となり信号再生装置が簡
略化され、コスト低減等の利点かある。
Furthermore, a current value control system is not required, the signal reproducing device is simplified, and there are advantages such as cost reduction.

〔発明の効果〕〔Effect of the invention〕

以上詳細に説明したごとく7本発明の磁気抵抗効果型ヘ
ッドによる信号再生方法と装置によれば。
As described above in detail, according to the method and apparatus for reproducing signals using a magnetoresistive head according to the present invention.

ヘッド作製工程上避けがたいヘッド特性のばらつき、特
にバイアス磁界の変動による再生信号波形の非対称性、
出力の変動を低減することができる。
Variations in head characteristics that are unavoidable during the head manufacturing process, especially asymmetry in the reproduced signal waveform due to fluctuations in the bias magnetic field.
Fluctuations in output can be reduced.

例えば、従来の装置では、再生信号波形の非対称度は5
〜35%と大きくばらついていたが1本発明の装置では
、全てのヘッドで非対称度を5%以下とすることができ
た。また、トラック@1μmと狭トラツクの磁気抵抗効
果型ヘッドにおいても。
For example, in a conventional device, the degree of asymmetry of the reproduced signal waveform is 5.
However, with the device of the present invention, the degree of asymmetry could be reduced to 5% or less for all heads. Also, in a magnetoresistive head with a narrow track of 1 μm.

本発明の信号再生方法および装置を用いることにより、
再生信号波形の非対称度を上記と同等に低下させること
ができた。
By using the signal reproducing method and device of the present invention,
The degree of asymmetry of the reproduced signal waveform could be reduced to the same level as above.

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

第1図および第2図は本発明の実施例1において例示し
た再生信号波形の非対称性制御系統図。 第3図は実施例2において例示した再生信号波形の非対
称性制御系統図、第4図は実施例3において例示した再
生信号波形の非対称性制御系統図。 第5図は従来のシャントバイアス型ヘッドの構成の一例
を示す模式図、第6図は従来の磁気抵抗効果型ヘッドの
出力−磁界曲線を示すグラフ、第7図は従来の差動型の
磁気抵抗効果型ヘッドの構成の一例を示す模式図である
。 1・・記録媒体 2・・・磁気抵抗効果型ヘッド 3・・・アンプ 4・・・波形非対称度検出部 5・・・比較部      6・・センス電源7・・・
プラスピークホールド部 8・マイナスピークホールド部 9 ・差動増幅部 10・・プラス側ピーク値検出部 11.12・・平均値演算部 13・・・マイナス側ピーク値検出部 14・・・A/Dコンバータ ↓5・・・メモリ 16・・・D/Aコンバータ 17・・・感磁部     18・・・電極19・・・
磁気抵抗効果膜 20・・・シャントバイアス膜 21・・−シールド膜   22・・・信号磁界23・
・・再生出力    24,25.26・・端子代理人
弁理士  中 村 純之助 4−−−ミ皮形非対称厚検出部 第1図 1−一一一記銖婦体 2−−一−胤気抵a効果型へ、7ド 3−−−−ア)ア 4−−−−:、皮形41:ff杯席檜出部5−−−−比
較部 6−−−−セレスを涜 7−−−−アラスl:a−7ホールド部8−一一一マイ
ナスぴ−7ホールド部 9−−−−寿1力糟中あl 第2図 1−一一一詑餘媒体 2−一一一扁【気おJ九効果型へ・・lド3−m−−7
レア 4−−一−シ皮竹3非丈寸オ竿J(オ剣tヒ苦い5−−
m−比較部 6−−−−e’、入電i獣 +4−−−−A/Dコンハ゛−7 !5−−−−メモ1) +6−−− D/Aコンノぐ−2 第4図 第5図
FIGS. 1 and 2 are system diagrams for controlling the asymmetry of the reproduced signal waveform illustrated in Embodiment 1 of the present invention. FIG. 3 is a system diagram for controlling the asymmetry of the reproduced signal waveform illustrated in the second embodiment, and FIG. 4 is a diagram showing the asymmetry control system for the asymmetry of the reproduced signal waveform illustrated in the third embodiment. Figure 5 is a schematic diagram showing an example of the configuration of a conventional shunt bias type head, Figure 6 is a graph showing the output-magnetic field curve of a conventional magnetoresistive head, and Figure 7 is a graph of a conventional differential type magnetic head. FIG. 2 is a schematic diagram showing an example of the configuration of a resistive head. 1... Recording medium 2... Magnetoresistive head 3... Amplifier 4... Waveform asymmetry detection unit 5... Comparison unit 6... Sense power supply 7...
Plus peak hold section 8・Minus peak hold section 9 ・Differential amplification section 10 . . . Plus side peak value detection section 11.12 .. Average value calculation section 13 . . . Minus side peak value detection section 14 . . A/ D converter↓5...Memory 16...D/A converter 17...Magnetic sensitive part 18...Electrode 19...
Magnetoresistive film 20... Shunt bias film 21...-Shield film 22... Signal magnetic field 23...
... Reproduction output 24, 25, 26 ... Terminal agent Patent attorney Junnosuke Nakamura 4 --- Skin shape asymmetric thickness detection section 1 Figure 1-111 Musai body 2 --- 1-Taneki resistance To the a effect type, 7 do 3 ---- a) a 4 ----:, skin shape 41: ff cup seat hinoki part 5 ---- comparison part 6 ---- Ceres 7 - - --Aras l: a-7 hold part 8-111 minus pi-7 hold part 9---Kotobuki 1 power medium Fig. 2 1-111 cover medium 2-111 [To the J9 effect type...ldo3-m--7
Rare 4--1-shihide bamboo 3 non-length O-rod J (O-ken Thi bitter 5--
m-comparison unit 6---e', incoming power i beast +4---A/D converter-7! 5----Memo 1) +6---- D/A Connog-2 Figure 4 Figure 5

Claims (1)

【特許請求の範囲】 1、磁気抵抗効果型ヘッドを用いて記録媒体に記録され
ている情報を再生する信号再生装置において、磁気抵抗
効果膜に印加されるバイアス磁界の強度を変えて磁気抵
抗効果膜の磁化方向を最適化する手段を設けたことを特
徴とする信号再生装置。 2、請求の範囲第1項記載の磁気抵抗効果型ヘッドを用
いた信号再生装置において、信号波形の非対称度を検出
する手段と、上記信号波形の非対称度に対応して磁気抵
抗効果膜への通電電流値を変えることにより、バイアス
磁界の強度を変えて磁気抵抗効果膜の磁化方向を最適化
する手段を設けたことを特徴とする信号再生装置。 3、請求の範囲第1項または第2項記載の磁気抵抗効果
型ヘッドを用いた信号再生装置において、信号波形の非
対称度を検出する手段は、信号波形のプラス側ピーク値
とマイナス側ピーク値との差を検出する手段によること
を特徴とする信号再生装置。 4、請求の範囲第1項、第2項または第3項記載の磁気
抵抗効果型ヘッドを用いた信号再生装置において、磁気
抵抗効果膜への通電電流値情報を、読み出し専用の半導
体メモリに記憶させておき、上記通電電流値情報をもと
にバイアス磁界の強度を変えて磁気抵抗効果膜の磁化方
向を最適化する手段を設けたことを特徴とする信号再生
装置。 5、請求の範囲第1項、第2項または第3項記載の信号
再生装置において、該信号再生装置の使用前に少なくと
も1度、磁気抵抗効果膜への通電電流値を最適化するよ
うに動作させる手段を設けたことを特徴とする信号再生
装置。 6、請求の範囲第5項記載の信号再生装置を用い、記録
媒体に1、0の信号を記録させ、該信号で信号波形のプ
ラス側ピーク値とマイナス側ピーク値との差を検出する
ことを特徴とする信号再生方法。 7、請求の範囲第6項記載の信号再生方法において、バ
イアス磁界の強度を変えて磁気抵抗効果膜の磁化方向を
最適化するための信号が、常に記録媒体に記録され保存
されていることを特徴とする信号再生方法。 8、請求の範囲第6項記載の信号再生方法において、バ
イアス磁界の強度を変えて磁気抵抗効果膜の磁化方向を
最適化するために用いる信号は、情報を再生するために
記録されている記録媒体の必要不可欠なデータからの信
号であることを特徴とする信号再生方法。 9、請求の範囲第1項ないし第5項のいずれか1項記載
の信号再生装置を備え、情報の記録および再生を行う手
段を有することを特徴とする記録装置。 10、請求の範囲第6項ないし第8項のいずれか1項記
載の信号再生方法を用いて、情報の記録および再生を行
うことを特徴とする記録方法。
[Claims] 1. In a signal reproducing device that reproduces information recorded on a recording medium using a magnetoresistive head, the magnetoresistive effect is achieved by changing the intensity of the bias magnetic field applied to the magnetoresistive film. A signal reproducing device characterized by comprising means for optimizing the magnetization direction of a film. 2. A signal reproducing device using a magnetoresistive head according to claim 1, including means for detecting the degree of asymmetry of the signal waveform, and means for detecting the degree of asymmetry of the signal waveform, and a means for detecting the degree of asymmetry of the signal waveform. 1. A signal reproducing device comprising means for optimizing the magnetization direction of a magnetoresistive film by changing the strength of a bias magnetic field by changing the value of a current. 3. In the signal reproducing device using the magnetoresistive head according to claim 1 or 2, the means for detecting the degree of asymmetry of the signal waveform detects the positive peak value and the negative peak value of the signal waveform. A signal reproducing device characterized by comprising means for detecting a difference between the two. 4. In a signal reproducing device using a magnetoresistive head according to claim 1, 2, or 3, information on the value of current flowing through the magnetoresistive film is stored in a read-only semiconductor memory. The signal reproducing device is further provided with a means for optimizing the magnetization direction of the magnetoresistive film by changing the strength of the bias magnetic field based on the current value information. 5. In the signal reproducing device according to claim 1, 2, or 3, the value of the current flowing through the magnetoresistive film is optimized at least once before using the signal reproducing device. A signal reproducing device characterized in that it is provided with means for operating it. 6. Recording a 1, 0 signal on a recording medium using the signal reproducing device according to claim 5, and detecting the difference between the positive peak value and the negative peak value of the signal waveform using the signal. A signal reproducing method characterized by: 7. In the signal reproducing method according to claim 6, the signal for optimizing the magnetization direction of the magnetoresistive film by changing the strength of the bias magnetic field is always recorded and stored in the recording medium. Characteristic signal reproduction method. 8. In the signal reproducing method as set forth in claim 6, the signal used for optimizing the magnetization direction of the magnetoresistive film by changing the strength of the bias magnetic field is a record recorded for reproducing information. A signal reproduction method characterized in that the signal is from essential data of a medium. 9. A recording device comprising the signal reproducing device according to any one of claims 1 to 5, and comprising means for recording and reproducing information. 10. A recording method characterized by recording and reproducing information using the signal reproducing method according to any one of claims 6 to 8.
JP33019390A 1990-11-30 1990-11-30 Method and device for reproducing signal by magnetoresistance effect type head and recording device using the same Pending JPH04205903A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP33019390A JPH04205903A (en) 1990-11-30 1990-11-30 Method and device for reproducing signal by magnetoresistance effect type head and recording device using the same

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP33019390A JPH04205903A (en) 1990-11-30 1990-11-30 Method and device for reproducing signal by magnetoresistance effect type head and recording device using the same

Publications (1)

Publication Number Publication Date
JPH04205903A true JPH04205903A (en) 1992-07-28

Family

ID=18229874

Family Applications (1)

Application Number Title Priority Date Filing Date
JP33019390A Pending JPH04205903A (en) 1990-11-30 1990-11-30 Method and device for reproducing signal by magnetoresistance effect type head and recording device using the same

Country Status (1)

Country Link
JP (1) JPH04205903A (en)

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH087203A (en) * 1994-06-22 1996-01-12 Internatl Business Mach Corp <Ibm> Driving method of mr head and hard-disk system
US5790335A (en) * 1995-03-13 1998-08-04 Fujitsu Limited Asymmetrical signal detector and signal regenerating apparatus using the same detector
US6067200A (en) * 1996-09-30 2000-05-23 Fujitsu Limited Method and apparatus for adjusting a bias current of a magneto-resistive effect type magnetic head and magnetic recording apparatus
US6297631B1 (en) * 1998-06-12 2001-10-02 Sony Corporation Magnetic signal reproducing method and apparatus using magneto-resistive effect element with increased sense current
JP2007200378A (en) * 2006-01-23 2007-08-09 Rohm Co Ltd Amplitude adjusting device and amplitude adjusting method, and storage system

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH087203A (en) * 1994-06-22 1996-01-12 Internatl Business Mach Corp <Ibm> Driving method of mr head and hard-disk system
US5790335A (en) * 1995-03-13 1998-08-04 Fujitsu Limited Asymmetrical signal detector and signal regenerating apparatus using the same detector
US6052245A (en) * 1995-03-13 2000-04-18 Fujitsu Limited Signal regenerating apparatus having asymmetrical signal detection circuit for detecting amplitude error and signal offset from a training signal and correcting same
US6067200A (en) * 1996-09-30 2000-05-23 Fujitsu Limited Method and apparatus for adjusting a bias current of a magneto-resistive effect type magnetic head and magnetic recording apparatus
US6297631B1 (en) * 1998-06-12 2001-10-02 Sony Corporation Magnetic signal reproducing method and apparatus using magneto-resistive effect element with increased sense current
JP2007200378A (en) * 2006-01-23 2007-08-09 Rohm Co Ltd Amplitude adjusting device and amplitude adjusting method, and storage system

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