JPH02208805A - System for reproducing magnetic record - Google Patents

System for reproducing magnetic record

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Publication number
JPH02208805A
JPH02208805A JP2952289A JP2952289A JPH02208805A JP H02208805 A JPH02208805 A JP H02208805A JP 2952289 A JP2952289 A JP 2952289A JP 2952289 A JP2952289 A JP 2952289A JP H02208805 A JPH02208805 A JP H02208805A
Authority
JP
Japan
Prior art keywords
magnetic
layer
reproducing
thin film
coil 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
JP2952289A
Other languages
Japanese (ja)
Inventor
Yoshio Koshikawa
越川 誉生
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.)
Fujitsu Ltd
Original Assignee
Fujitsu 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 Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP2952289A priority Critical patent/JPH02208805A/en
Publication of JPH02208805A publication Critical patent/JPH02208805A/en
Pending legal-status Critical Current

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

Abstract

PURPOSE:To obtain a reproducing output waveform with satisfactory symmetric property for positive and negative waveforms by adding reproducing output generated by an inductive voltage at a coil layer on the reproducing generated by a magneto- resistance effect element at the time of reproducing information on a magnetic recording medium recorded by the coil layer. CONSTITUTION:A recording and reproducing magnetic head 11 is structured in such a way that a first magnetic layer 14, the coil layer 16 sandwiched between a gap layer 16 and an inter-layer insulation layer 15, a second magnetic layer 17, and a protection layer 18 are laminated sequentially on a nonmagnetic substrate 12, and also, a thin film magneto-resistance effect element(thin film MR element) 19 is arranged in the gap layer 14. And the reproduction of the recording information of a confronting magnetic recording medium 20 by the thin film MR element 19 and that by the inductive voltage at the coil layer 16 are performed simultaneously by the magnetic recording and reproducing head 11. Since the phase of the reproducing output waveform 21 by the thin film MR element 19 is equivalent to that of the reproducing output waveform 22 by the coil layer 16, both reproducing output are synthesized at an adder circuit 23. Thereby, the symmetric property of positive and negative waveforms of a synthesized reproducing output waveform 24 can be improved, and the recording information can accurately be reproduced.

Description

【発明の詳細な説明】 〔概 要] 磁気ディスク装置や磁気テープ装置に用いられる磁気記
録情報の再生方式、特に磁極ギャップ部に記録磁界を発
生させるコイル層と再生専用磁気〔産業上の利用分野〕 本発明は磁気ディスク装置や磁気テープ装置に用いられ
る磁気記録情報の再生方式に関わり、特に磁極ギャップ
部に記録磁界を発生させるコイル層と再生専用磁気抵抗
効果素子とを備えた磁気へラドを用いた磁気記録の再生
方式に関するものである。
[Detailed description of the invention] [Summary] A method for reproducing magnetically recorded information used in a magnetic disk device or a magnetic tape device, particularly a coil layer that generates a recording magnetic field in the magnetic pole gap portion and a reproduction-only magnet [Industrial application field] ] The present invention relates to a method for reproducing magnetically recorded information used in a magnetic disk device or a magnetic tape device, and particularly relates to a magnetic helad that is equipped with a coil layer that generates a recording magnetic field in the magnetic pole gap portion and a read-only magnetoresistive element. This paper relates to the magnetic recording reproduction method used.

近年、磁気記録の高密度化に伴い、高出力で良好な再生
波形が安定に得ら・れる記録再生方式が要求されている
。再生専用の薄膜磁気抵抗効果素子(以下MR素子と略
称する)による磁気ヘッドの再生出力は記録媒体の移動
速度に依存しないため、特にその移動速度が低い場合に
はコイル層を用いたインダクティブ型の記録再生用磁気
ヘッドよりも大出力が得易いことから磁気記録再生装置
の小型化に伴って有望視されているが、薄膜により形成
されるMR素子自体の磁気特性や形状のばらつき等によ
って磁気記録情報の再生時に良好な再生波形が得られ難
い傾向がある。このため、磁気記録情報の再生時に良好
な再生波形が得られ、かつその記録情報を正確に再生す
ることができる方式が必要とされている。
In recent years, with the increase in the density of magnetic recording, there has been a demand for a recording/reproducing method that can stably obtain high output and good reproduced waveforms. The reproduction output of a magnetic head using a read-only thin film magnetoresistive element (hereinafter abbreviated as MR element) does not depend on the moving speed of the recording medium, so if the moving speed is particularly low, an inductive type using a coil layer is recommended. It is seen as promising as magnetic recording and reproducing devices become smaller because it is easier to obtain larger output than magnetic heads for recording and reproducing, but due to variations in the magnetic properties and shape of the MR element itself formed from a thin film, When reproducing information, it tends to be difficult to obtain a good reproduced waveform. Therefore, there is a need for a method that can obtain a good reproduction waveform when reproducing magnetically recorded information and can accurately reproduce the recorded information.

〔従来の技術〕[Conventional technology]

従来の記録再生方式は、例えばコイル層の両側に眉間絶
縁層を介して磁極層が配置され、かつその両磁極先端間
のギャップ内に薄膜磁気抵抗効果素子(以下MR素子と
略称する)が配設された構造の記録再生磁気ヘッドを用
い、対向する磁気記録媒体に情報を記録する場合には、
前記磁気ヘッドのコイル層に記録情報の信号電流を通電
して前記第一、第二磁極層を磁化し、ギャップ層を挟む
前記両磁極層の先端部から漏出する磁界によって記録を
行う。また逆に磁気記録媒体に記録された情報を再生す
る場合には、該媒体からの漏洩磁界により変化する前記
ギャップ層内の薄膜MR素子の抵抗値を電圧変化として
検出して再生出力を得るようにして、前記磁気記録媒体
に対する情報の書き込みと読み出しを分担している。
In the conventional recording and reproducing method, for example, magnetic pole layers are arranged on both sides of a coil layer with an insulating layer between the eyebrows interposed therebetween, and a thin film magnetoresistive element (hereinafter abbreviated as MR element) is arranged in the gap between the tips of the two magnetic poles. When recording information on an opposing magnetic recording medium using a recording/reproducing magnetic head having a structure,
A signal current for recording information is applied to the coil layer of the magnetic head to magnetize the first and second magnetic pole layers, and recording is performed by a magnetic field leaking from the tips of the two magnetic pole layers sandwiching the gap layer. Conversely, when reproducing information recorded on a magnetic recording medium, the resistance value of the thin film MR element in the gap layer, which changes due to the leakage magnetic field from the medium, is detected as a voltage change to obtain a reproduction output. They share the task of writing and reading information to and from the magnetic recording medium.

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

ところで上記したような従来の記録再生用磁気ヘッドに
おける薄膜MR素子によって磁気記録媒体の記録情報の
再生時における再生出力波形は、本来、第5図に示すよ
うに0■ラインを中心にして正負の波形が対称となる良
好な波形が得られるが、該薄膜MR素子自体の磁気特性
やパターニング形成による素子形状のバラツキ等によっ
て、最適バイアス点がずれる等の再生特性のバラツキが
発生し易く、例えば第6図に示すようなOvラインを中
心にして正負の波形が非対称な再生波形となる場合があ
る。このため再生波形にピークシフトが発生して、記録
情報の正確な再生が困難となるという問題があった。
By the way, when the thin film MR element in the conventional recording/reproducing magnetic head described above reproduces information recorded on a magnetic recording medium, the reproduced output waveform originally has positive and negative polarities centered on the 0■ line, as shown in FIG. Although a good waveform with a symmetrical waveform can be obtained, due to the magnetic properties of the thin film MR element itself and variations in the element shape due to patterning, variations in reproduction characteristics such as shifts in the optimum bias point are likely to occur. There are cases where the reproduced waveform has an asymmetrical positive and negative waveform around the Ov line as shown in FIG. This causes a problem in that a peak shift occurs in the reproduced waveform, making it difficult to accurately reproduce recorded information.

本発明は上記した従来の問題点に鑑み、薄膜MR素子を
用いた記録再生磁気ヘッドにより磁気記録媒体の記録情
報を再生する際に、該薄膜MR素子の磁気特性や素子形
状等のバラツキが多少あっても、正負の波形の対称性が
良好な再生出力波形を得ることができる新規な磁気記録
の再生方式を提供することを目的とするものである。
In view of the above-mentioned conventional problems, the present invention has been developed to solve the problem that, when reproducing information recorded on a magnetic recording medium using a recording/reproducing magnetic head using a thin film MR element, there is some variation in the magnetic properties, element shape, etc. of the thin film MR element. The object of the present invention is to provide a novel magnetic recording reproduction method that can obtain a reproduced output waveform with good symmetry between positive and negative waveforms.

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

本発明は上記した目的を達成するため、磁気記録媒体に
情報を記録するための磁極ギャップ部に記録磁界を発生
させるコイル層と、情報再生専用の薄膜磁気抵抗効果素
子とを備えた磁気ヘッドにおいて、前記コイル層により
記録した磁気記録媒体上の情報を再生する際に、前記磁
気抵抗効果素子による再生出力に前記コイル層での誘起
電圧による再生出力を加算する構成とする。
In order to achieve the above object, the present invention provides a magnetic head equipped with a coil layer that generates a recording magnetic field in a magnetic pole gap portion for recording information on a magnetic recording medium, and a thin film magnetoresistive element dedicated to information reproduction. When reproducing information on a magnetic recording medium recorded by the coil layer, a reproduction output due to an induced voltage in the coil layer is added to a reproduction output by the magnetoresistive element.

〔作 用〕[For production]

本発明によれば、情報を記録するための磁極ギャップ部
に記録磁界を発生させるコイル層と、情報再生専用の薄
膜MR素子とを備えた磁気ヘッドにより磁気記録媒体の
記録情報を再生する場合、前記薄膜MR素子による再生
の他に、記録磁界を発生させるコイル層での誘起電圧に
よる再生が可能であり、しかもその再生出力波形はO■
ラインを中心にして正負の波形の対称性が良いことを利
用して、薄膜MR素子による再生出力に、前記コイル層
による正負波形の対称性の良い再生出力を加えて合成す
ることにより、例え磁気特性や素子形状等のバラツキに
より該薄膜MR素子による再主出力波形の正負波形が非
対称性であっても、前記合成再生出力波形の正負波形の
対称度が改善され、記録情報の正確な再生が可能となる
According to the present invention, when reproducing information recorded on a magnetic recording medium using a magnetic head including a coil layer that generates a recording magnetic field in a magnetic pole gap portion for recording information and a thin film MR element exclusively for reproducing information, In addition to reproduction using the thin film MR element, reproduction can be performed using the induced voltage in the coil layer that generates the recording magnetic field, and the reproduction output waveform is O■
Taking advantage of the fact that the positive and negative waveforms have good symmetry around the line, the reproduction output from the thin film MR element is combined with the reproduction output from the coil layer, which has good symmetry between the positive and negative waveforms. Even if the positive and negative waveforms of the re-main output waveform from the thin film MR element are asymmetrical due to variations in characteristics, element shape, etc., the degree of symmetry of the positive and negative waveforms of the composite reproducing output waveform is improved, and accurate reproduction of recorded information is possible. It becomes possible.

〔実施例〕〔Example〕

以下図面を用いて本発明の実施例について詳細に説明す
る。
Embodiments of the present invention will be described in detail below with reference to the drawings.

第1図は本発明に係る磁気記録の再生方式に用いる記録
再生用磁気ヘッドの一例を示す要部縦断面図である。
FIG. 1 is a longitudinal sectional view of a main part showing an example of a recording/reproducing magnetic head used in the magnetic recording/reproducing method according to the present invention.

本実施例では図示のように、スライダとなる非磁性基板
12上に第一磁極層13とギャップ層14及び層間絶縁
層15で挾まれたコイル層16、第二磁極層17、保護
層18が順に積層され、かつ該ギャップ層14内に薄膜
磁気抵抗効果素子(以下薄膜MR素子と略称する)19
が配設された構造の記録再生磁気へラド11により、対
向する磁気記録媒体20の記録情報を該薄膜MR素子1
9による再生と、コイル層16での誘起電圧による再生
とを同時に行う。
In this embodiment, as shown in the figure, a coil layer 16, a second magnetic pole layer 17, and a protective layer 18 are sandwiched between a first magnetic pole layer 13, a gap layer 14, and an interlayer insulating layer 15 on a nonmagnetic substrate 12 serving as a slider. A thin film magnetoresistive element (hereinafter abbreviated as thin film MR element) 19 is laminated in this order and is disposed within the gap layer 14.
A recording/reproducing magnetic head 11 having a structure in which
The reproduction by the coil layer 16 and the reproduction by the induced voltage in the coil layer 16 are performed simultaneously.

この際の薄膜MR素子19による再生出力波形21と前
記コイル層16による再生出力波形22は第2図に示す
ように同位相であるため、その両再生出力を加算回路2
3にて合成する。
At this time, since the reproduced output waveform 21 from the thin film MR element 19 and the reproduced output waveform 22 from the coil layer 16 are in the same phase as shown in FIG.
Synthesize in step 3.

このようにすれば、例えば該薄膜MR素子19による再
生出力波形21の正負の再生出力値を各々a。
In this way, for example, the positive and negative reproduction output values of the reproduction output waveform 21 by the thin film MR element 19 are set to a, respectively.

b、該コイル層16による再生出力波形22の正、また
は負の再生出力値をCとし、その各正負の再生出力値a
、b、cの比率を、a −0,8+  b = 1 +
  c=0.5とした場合、前記薄膜MR素子19によ
る再生出力波形21の正負出力比はa / b =0.
8となるが、前記加算回路23にて合成された合成再生
出力波形24の正負再生出力比は(b + c)/(a
 + c)=1.3/1゜5−0.87となり、該合成
再生出力波形24の正負波形の対称度が改善される。従
って、記録情報を正確に再生することができる。
b. Let C be the positive or negative reproduction output value of the reproduction output waveform 22 by the coil layer 16, and let each positive or negative reproduction output value a
, b, c, a −0,8+ b = 1 +
When c=0.5, the positive/negative output ratio of the reproduced output waveform 21 from the thin film MR element 19 is a/b=0.
8, but the positive/negative reproduction output ratio of the composite reproduction output waveform 24 synthesized by the adding circuit 23 is (b + c)/(a
+c)=1.3/1°5-0.87, and the symmetry of the positive and negative waveforms of the composite reproduced output waveform 24 is improved. Therefore, recorded information can be accurately reproduced.

また第3図は本発明に係る磁気記録の再生方式に用いる
記録再生用磁気ヘッドの他の例を示す要部縦断面図であ
り、第1図と同等部分には同一符号を付している。
Further, FIG. 3 is a longitudinal cross-sectional view of a main part showing another example of a magnetic recording/reproducing head used in the magnetic recording/reproducing method according to the present invention, and parts equivalent to those in FIG. 1 are given the same reference numerals. .

本実施例では図示のように、例えば磁気シールドを兼ね
る磁性基板42上に非磁性絶縁層43を介して薄膜MR
素子44が配設され、その上に第一磁極層13とギャッ
プ層14及び層間絶縁層15で挟まれたコイル層16、
第二磁極層17、保護層18が順に積層された構造の記
録再生磁気ヘッド41により、対向する磁気記録媒体2
0の記録情報を該薄膜MR素子44による再生と、コイ
ルIJ16での誘起電圧による再生とを同時に行う。
In this embodiment, as shown in the figure, a thin film MR is formed on a magnetic substrate 42 which also serves as a magnetic shield, with a non-magnetic insulating layer 43 interposed therebetween.
A coil layer 16 on which the element 44 is disposed and sandwiched between the first magnetic pole layer 13, the gap layer 14, and the interlayer insulating layer 15;
A recording/reproducing magnetic head 41 having a structure in which a second magnetic pole layer 17 and a protective layer 18 are laminated in this order is used to oppose a magnetic recording medium 2.
The recorded information of 0 is simultaneously reproduced by the thin film MR element 44 and by the induced voltage in the coil IJ16.

この場合には、前記磁気ヘッド41における薄膜MR素
子44がギャップ層14外の磁性基板42と第一磁極層
13との間に設けられているため、該薄膜MR素子44
による再生出力波形51と前記コイル層16による再生
出力波形52とに位相差が生じる。
In this case, since the thin film MR element 44 in the magnetic head 41 is provided between the magnetic substrate 42 outside the gap layer 14 and the first magnetic pole layer 13, the thin film MR element 44
A phase difference occurs between the reproduced output waveform 51 caused by the coil layer 16 and the reproduced output waveform 52 generated by the coil layer 16.

従って、第4図に示すようにその両再生出力を加算回路
23にて合成するに際し、例えば薄膜MR素子44によ
る再生出力を遅延回路53へ送ってコイル層16による
再生出力波形52との位相を調整した後に、その両再生
出力を前記加算回路23で合成して正負波形の対称度の
良好な合成再生出力波形54を得るようにする。このよ
うな実施例によっても記録情報を正確に再生できる。
Therefore, as shown in FIG. 4, when the two reproduced outputs are combined in the adder circuit 23, the reproduced output from the thin film MR element 44 is sent to the delay circuit 53, and the phase with the reproduced output waveform 52 from the coil layer 16 is adjusted. After the adjustment, both reproduced outputs are combined by the adder circuit 23 to obtain a combined reproduced output waveform 54 with good symmetry between positive and negative waveforms. Such an embodiment also allows recorded information to be reproduced accurately.

なお、以上の実施例では磁気ヘッドに対する磁気記録媒
体の走行方向が、該磁気ヘッドの薄膜MR素子側より磁
掻ギャップ側へ方向に磁気記録媒体が走行する場合の例
で説明したが、該記録媒体の走行方向が逆の場合には、
コイル層による再生出力側に遅延回路を設置して前記再
再生出力波形の位相を調整するようにすればよい。
Note that in the above embodiments, the running direction of the magnetic recording medium with respect to the magnetic head is explained as an example in which the magnetic recording medium runs in a direction from the thin film MR element side of the magnetic head to the magnetic scratching gap side. If the direction of media travel is reversed,
A delay circuit may be installed on the reproduction output side of the coil layer to adjust the phase of the reproduction output waveform.

(発明の効果〕 以上の説明から明らかなように、本発明に係る磁気記録
の再生方式によれば、磁気特性や形状のバラツキ等で薄
膜MR層素子による再生出力波形の正負波形が非対称性
となっても、コイル層による正負波形の対称性が良い再
生出力波形との合成により正負波形の対称性の良い合成
再生出力波形が容易に得られ、正確な記録情報の再生が
可能となる等、実用上の効果は大きい。
(Effects of the Invention) As is clear from the above explanation, according to the magnetic recording reproducing method according to the present invention, the positive and negative waveforms of the reproduced output waveform by the thin film MR layer element become asymmetric due to variations in magnetic properties and shape. However, by combining the reproduced output waveform with good symmetry between positive and negative waveforms using the coil layer, a composite reproduced output waveform with good symmetry between positive and negative waveforms can be easily obtained, making it possible to accurately reproduce recorded information, etc. The practical effects are significant.

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

第1図は本発明に係る磁気記録の再生方式に用いる記録
再生用磁気ヘッドの一例を示 す要部縦断面図、 第2図は本発明に係る磁気記録の再生方式の一実施例を
示す説明図、 第3図は本発明に係る磁気記録の再生方式に用いる記録
再生用磁気ヘッドの他の例を 示す要部縦断面図、 第4図は本発明に係る磁気記録の再生方式の他の実施例
を示す説明図、 第5図は薄膜MR素子による本来の正常な再生出力波形
を示す図、 第6図は薄膜MR素子による正負波形が非対称な再生出
力波形を示す図である。 第1図〜第4図において、 IL 41は磁気ヘッド、12は非磁性基板、13は第
一磁極層、14はギャップ層、15は眉間絶縁層、16
はコイル層、17は第二磁極層、18は保護層、19.
44は薄膜MR素zトW!B月−−1タヒハl;月11
・)#ノ1へ〜ト)−看tト自ブT;1′喝芦茅p許’
rtη−1b図第1図 本祁萌偽4オ収「實飽伊厖木tα研m 第2図 子、20は磁気記録媒体、21.22.51.52は再
生出力波形、23は加算回路、24.54は合成再生出
力波形、42は磁性基板、43は非磁性絶縁層、53は
遅延回路をそれぞれ示す。 本例/1酊プ1文r1賃(・磁気へ・7F室でQクツシ
ネττ−FISJすを新面GO第 3 図 クト$IIQFI士方)\の台−♂ス乙か(イ准木す哀
lOg図第4図
FIG. 1 is a longitudinal cross-sectional view of a main part showing an example of a magnetic head for recording and reproducing used in the magnetic recording reproducing method according to the present invention, and FIG. 2 is an explanation showing an embodiment of the magnetic recording reproducing method according to the present invention. 3 is a vertical sectional view of a main part showing another example of a magnetic head for recording and reproducing used in the magnetic recording reproducing method according to the present invention, and FIG. 4 is a longitudinal sectional view of another example of a magnetic recording reproducing method according to the present invention. FIG. 5 is a diagram showing an original normal reproduction output waveform of the thin film MR element; FIG. 6 is a diagram showing an asymmetric reproduction output waveform of positive and negative waveforms of the thin film MR element. 1 to 4, IL 41 is a magnetic head, 12 is a non-magnetic substrate, 13 is a first magnetic pole layer, 14 is a gap layer, 15 is an insulating layer between eyebrows, 16
17 is a coil layer, 17 is a second magnetic pole layer, 18 is a protective layer, 19.
44 is a thin film MR element W! Month B--1 Tahiha; Month 11
・) Go to #ノ1~ト) -Watch your own
rtη-1b Diagram 1 Honke Moe False 4O Collection "Jiku Ikuiki tα Lab" Figure 2, 20 is the magnetic recording medium, 21.22.51.52 is the playback output waveform, 23 is the addition circuit , 24.54 shows the composite reproduction output waveform, 42 shows the magnetic substrate, 43 shows the non-magnetic insulating layer, and 53 shows the delay circuit. ττ-FISJ Suwo Shinmen GO Figure 3 Kuto $IIQFI Shikata) \'s stand-♂Suotsuka (I Junkisu Sad lOg Figure 4)

Claims (1)

【特許請求の範囲】 磁気記録媒体(20)に情報を記録するための磁極ギャ
ップ部に記録磁界を発生させるコイル層(16)と、情
報再生専用の薄膜磁気抵抗効果素子(19)とを備えた
磁気ヘッド(11)において、 上記コイル層(16)により記録した磁気記録媒体(2
0)上の情報を再生する際に、前記磁気抵抗効果素子(
19)による再生出力に前記コイル層(16)での誘起
電圧による再生出力を加算することを特徴とする磁気記
録の再生方式。
[Claims] A magnetic recording medium (20) includes a coil layer (16) that generates a recording magnetic field in a magnetic pole gap portion for recording information, and a thin film magnetoresistive element (19) dedicated to information reproduction. In the magnetic head (11), a magnetic recording medium (2) recorded by the coil layer (16) is provided.
0) When reproducing information on the magnetoresistive element (
19) A reproduction method for magnetic recording characterized in that a reproduction output due to an induced voltage in the coil layer (16) is added to the reproduction output obtained by the coil layer (16).
JP2952289A 1989-02-07 1989-02-07 System for reproducing magnetic record Pending JPH02208805A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2952289A JPH02208805A (en) 1989-02-07 1989-02-07 System for reproducing magnetic record

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2952289A JPH02208805A (en) 1989-02-07 1989-02-07 System for reproducing magnetic record

Publications (1)

Publication Number Publication Date
JPH02208805A true JPH02208805A (en) 1990-08-20

Family

ID=12278436

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2952289A Pending JPH02208805A (en) 1989-02-07 1989-02-07 System for reproducing magnetic record

Country Status (1)

Country Link
JP (1) JPH02208805A (en)

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