JPH06301934A - Magnetic recording/reproducing apparatus - Google Patents
Magnetic recording/reproducing apparatusInfo
- Publication number
- JPH06301934A JPH06301934A JP9278993A JP9278993A JPH06301934A JP H06301934 A JPH06301934 A JP H06301934A JP 9278993 A JP9278993 A JP 9278993A JP 9278993 A JP9278993 A JP 9278993A JP H06301934 A JPH06301934 A JP H06301934A
- Authority
- JP
- Japan
- Prior art keywords
- current
- magnetic field
- bias
- reproducing
- magnetic
- 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
- G11B5/02—Recording, reproducing, or erasing methods; Read, write or erase circuits therefor
-
- 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
- G11B2005/0002—Special dispositions or recording techniques
- G11B2005/0005—Arrangements, methods or circuits
- G11B2005/0008—Magnetic conditionning of heads, e.g. biasing
-
- 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
- G11B2005/0002—Special dispositions or recording techniques
- G11B2005/0005—Arrangements, methods or circuits
- G11B2005/001—Controlling recording characteristics of record carriers or transducing characteristics of transducers by means not being part of their structure
- G11B2005/0013—Controlling recording characteristics of record carriers or transducing characteristics of transducers by means not being part of their structure of transducers, e.g. linearisation, equalisation
- G11B2005/0016—Controlling recording characteristics of record carriers or transducing characteristics of transducers by means not being part of their structure of transducers, e.g. linearisation, equalisation of magnetoresistive transducers
- G11B2005/0018—Controlling recording characteristics of record carriers or transducing characteristics of transducers by means not being part of their structure of transducers, e.g. linearisation, equalisation of magnetoresistive transducers by current biasing control or regulation
Landscapes
- Magnetic Heads (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】本発明は磁気抵抗効果素子からな
る再生用ヘッドを具備した磁気記録再生装置に関するも
のである。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a magnetic recording / reproducing apparatus having a reproducing head composed of a magnetoresistive effect element.
【0002】[0002]
【従来の技術】近年、磁気記録分野において、高記録密
度化に伴い、狭トラック、マルチトラック化された薄膜
磁気ヘッドが必要となっている。この薄膜磁気ヘッドに
はバルクヘッドと同様にコイルを用いたインダクティブ
型ヘッドと磁気抵抗効果(MR効果)を利用した再生用
のMRヘッドが知られている。2. Description of the Related Art In recent years, in the field of magnetic recording, a thin track magnetic head having a narrow track and a multi track has been required as the recording density is increased. As this thin film magnetic head, an inductive head using a coil and a reproducing MR head utilizing a magnetoresistive effect (MR effect) are known as in a bulk head.
【0003】コイルを用いたインダクティブ型ヘッドは
その出力がテープ/ヘッドの相対速度に比例するため、
相対速度が小さい場合出力も小さくなり、良好な再生が
できない。一方、磁気抵抗効果(MR効果)を利用した
磁気抵抗効果型ヘッド(以下MRヘッドという)は、磁
気抵抗効果素子(以下MR素子という)に流入する磁束
に応じてその抵抗値が変化しこれにより電磁変換を行な
うため、テープ/ヘッドの相対速度に無関係に、高出力
が得られるという利点がある。Since the output of an inductive head using a coil is proportional to the relative speed of the tape / head,
When the relative speed is small, the output also becomes small, and good reproduction cannot be performed. On the other hand, a magnetoresistive head (hereinafter referred to as MR head) utilizing the magnetoresistive effect (MR effect) has its resistance value changed according to the magnetic flux flowing into the magnetoresistive effect element (hereinafter referred to as MR element). Since electromagnetic conversion is performed, there is an advantage that a high output can be obtained regardless of the relative speed of the tape / head.
【0004】MRヘッドは図4に示す断面構造を有す
る。つまり、磁性基板41上に絶縁層を介してバイアス
導体層42が形成され、さらに絶縁層を介してMR素子
43が形成されている。MR素子43にセンス電流を印
加するため、リード層(図示せず)がMR素子43の両
端に形成され、そして絶縁層を介して記録媒体44上の
信号磁界をMR素子43に印加するヨーク45が形成さ
れている。MRヘッドの前部ギャップ部46では絶縁層
によりギャップ長を規制し、後部ギャップ部47ではヨ
ーク45と磁性基板41が磁気的に結合している。The MR head has a sectional structure shown in FIG. That is, the bias conductor layer 42 is formed on the magnetic substrate 41 via the insulating layer, and the MR element 43 is further formed via the insulating layer. In order to apply a sense current to the MR element 43, lead layers (not shown) are formed at both ends of the MR element 43, and a yoke 45 for applying a signal magnetic field on the recording medium 44 to the MR element 43 via an insulating layer. Are formed. In the front gap portion 46 of the MR head, the gap length is regulated by the insulating layer, and in the rear gap portion 47, the yoke 45 and the magnetic substrate 41 are magnetically coupled.
【0005】再生過程について説明する。再生動作時、
バイアス導体層42にはバイアス電流と呼ばれる直流電
流が印加されており、この電流で生じる直流磁界により
バイアス点を設定し、このバイアス点を中心として記録
媒体からの信号磁界がヨーク45によりMR素子43に
印加され、この信号磁界によりMR素子43の抵抗が変
化し、この抵抗変化をリード層に流すセンス電流により
電圧変化として取り出す。バイアス点はこの電圧変化の
感度と、歪から決定される。The reproducing process will be described. During playback operation,
A direct current called a bias current is applied to the bias conductor layer 42. A direct current magnetic field generated by this current sets a bias point, and a signal magnetic field from the recording medium around this bias point is centered on the MR element 43 by the yoke 45. Applied to the MR element 43, the resistance of the MR element 43 changes due to this signal magnetic field, and this resistance change is extracted as a voltage change by the sense current flowing in the lead layer. The bias point is determined from the sensitivity of this voltage change and distortion.
【0006】[0006]
【発明が解決しようとする課題】上記従来の磁気記録再
生装置では再生時には磁壁の移動に起因するバルクハウ
ゼンノイズが発生し、良好な信号再生が阻害される。こ
れを以下に説明する。In the above-described conventional magnetic recording / reproducing apparatus, Barkhausen noise caused by the movement of the domain wall is generated during reproduction, and good signal reproduction is hindered. This will be explained below.
【0007】MR素子は通常、信号磁界の流入方向の直
角方向に磁化容易軸が形成されており、このとき、バイ
アス磁界が無い場合のMR素子内の磁化は磁化容易軸に
平行な方向を向くが、図5に示すようにMR素子42内
の磁気的な安定性のため磁壁48が発生している。In the MR element, an easy axis of magnetization is usually formed in a direction perpendicular to the inflow direction of the signal magnetic field. At this time, the magnetization in the MR element in the absence of a bias magnetic field is oriented in a direction parallel to the easy axis of magnetization. However, as shown in FIG. 5, the magnetic domain wall 48 is generated due to the magnetic stability in the MR element 42.
【0008】このような状態でバイアス電流、センス電
流を印加し再生動作状態とすると、磁壁の不連続移動が
生じこれがバルクハウゼンノイズとなり良好な再生が阻
害されるという問題があった。When a reproducing current is applied by applying a bias current and a sense current in such a state, there is a problem that a discontinuous movement of the domain wall occurs and this becomes Barkhausen noise, which hinders good reproduction.
【0009】本発明は上記問題点を解決し、バルクハウ
ゼンノイズの無い良好な信号の再生を行なう磁気記録再
生装置を提供することを目的とする。An object of the present invention is to solve the above problems and to provide a magnetic recording / reproducing apparatus which reproduces a good signal without Barkhausen noise.
【0010】[0010]
【課題を解決するための手段】この目的を達成するた
め、本発明の磁気記録再生装置はMR素子の磁化容易軸
方向がMR素子に流入する信号磁界の流入方向の直角方
向に対し5〜30度傾いたMR素子と、前記MR素子に
バイアス磁界を印加するバイアス導体を有し、前記バイ
アス導体に直流電流I1 を印加したのち連続的に電流値
をI2 (I1>I2>0)に変化させる直流電流回路を具
備することを特徴とする。電流I2 はこれによって生じ
る磁界によりMR素子の出力の感度、歪が良好となる電
流である。To achieve this object, in the magnetic recording / reproducing apparatus of the present invention, the easy axis of magnetization of the MR element is 5 to 30 with respect to the direction perpendicular to the inflow direction of the signal magnetic field flowing into the MR element. It has a tilted MR element and a bias conductor for applying a bias magnetic field to the MR element, and after applying a direct current I 1 to the bias conductor, the current value is continuously changed to I 2 (I 1 > I 2 > 0). ) Is included in the DC current circuit. The current I 2 is a current in which the sensitivity and distortion of the output of the MR element are improved by the magnetic field generated thereby.
【0011】[0011]
【作用】本発明は上記した構成により、直流電流I1 を
印加した際、単磁区状態ができるためMR素子内に磁壁
が発生せず、従ってバルクハウゼンノイズのない良好な
信号再生ができる。According to the present invention, when the direct current I 1 is applied, a single domain state can be formed by the above-described structure, so that no domain wall is generated in the MR element, and therefore good signal reproduction without Barkhausen noise can be performed.
【0012】[0012]
【実施例】以下に本発明の実施例について説明する。EXAMPLES Examples of the present invention will be described below.
【0013】図1は本発明による磁気記録再生装置の再
生部の構成図である。1はMRヘッド、2はMRヘッド
1のバイアス導体層にバイアス電流を印加する電流回
路、3はMRヘッド1中のMR素子にセンス電流を印加
し、再生出力を検知する再生回路、5はバイアス導体
層、6はMR素子である。記録系のヘッド及び回路、記
録媒体を走行させる機構等については省略する。FIG. 1 is a block diagram of a reproducing section of a magnetic recording / reproducing apparatus according to the present invention. Reference numeral 1 is an MR head, 2 is a current circuit for applying a bias current to a bias conductor layer of the MR head 1, 3 is a reproducing circuit for applying a sense current to an MR element in the MR head 1, and a reproducing circuit for detecting a reproduction output, and 5 is a bias. The conductor layer 6 is an MR element. The heads and circuits of the recording system, the mechanism for moving the recording medium, etc. are omitted.
【0014】図2はMRヘッドの断面図である。磁性基
板4上に絶縁層を介して、バイアス導体層5が形成され
ている。バイアス導体層5はバイアス磁界を印加するた
めに電流を印加する電流回路2に接続されている。さら
に絶縁層を介してMR素子6が形成されている。MR素
子6にセンス電流を印加するため、リード層(図示せ
ず)がMR素子6の両端に形成されている。リード層は
MR素子6の抵抗変化を検知する再生回路3に接続され
ている。そして絶縁層を介して記録媒体7上の信号磁界
をMR素子6に印加するヨーク8が形成されている。M
Rヘッドの前部ギャップ部9では絶縁層によりギャップ
長を規制し、後部ギャップ部10ではヨーク8と磁性基
板4が磁気的に結合している。FIG. 2 is a sectional view of the MR head. The bias conductor layer 5 is formed on the magnetic substrate 4 via an insulating layer. The bias conductor layer 5 is connected to the current circuit 2 that applies a current to apply a bias magnetic field. Further, the MR element 6 is formed via the insulating layer. Lead layers (not shown) are formed at both ends of the MR element 6 in order to apply a sense current to the MR element 6. The lead layer is connected to the reproducing circuit 3 which detects a resistance change of the MR element 6. Then, a yoke 8 for applying a signal magnetic field on the recording medium 7 to the MR element 6 via an insulating layer is formed. M
In the front gap portion 9 of the R head, the gap length is regulated by the insulating layer, and in the rear gap portion 10, the yoke 8 and the magnetic substrate 4 are magnetically coupled.
【0015】次に再生時の動作について簡単に説明す
る。まず、MRヘッドの出力の感度、歪を勘案して、最
適バイアス点を与える磁界を生ぜしむため、バイアス導
体層5に印加する直流電流値をI2 とする。Next, the operation during reproduction will be briefly described. First, in consideration of the sensitivity and distortion of the output of the MR head, a direct current value applied to the bias conductor layer 5 is set to I 2 in order to generate a magnetic field that gives an optimum bias point.
【0016】再生動作の開始時にはバイアス導体層5に
電流I1 (>I2 )が一定時間印加され、そして、電流
値をI2 まで連続的に減少させ、その後、電流値をI2
を定常的に印加する。The current I 1 to the bias conductor layer 5 at the start of the reproducing operation (> I 2) is applied a predetermined time, and reduces the current value continuously to I 2, then the current value I 2
Is constantly applied.
【0017】また、リード層にはMR素子の抵抗変化を
検知するため、センス電流が再生回路3から印加されて
いる。A sense current is applied to the lead layer from the reproducing circuit 3 in order to detect a change in resistance of the MR element.
【0018】バイアス導体層5に電流値をI2 が定常的
に印加されている状態の時、記録媒体7上の信号磁界が
MRヘッドの前部ギャップ部9から流入し、この信号磁
界がヨーク8、MR素子6、磁性基板4からなる磁気回
路を流れる。MR素子6において信号磁界の強度に対応
してMR素子の抵抗が変化することにより電磁変換が行
なわれ、リード層により、その読みだしが行なわれる。When the current value I 2 is constantly applied to the bias conductor layer 5, the signal magnetic field on the recording medium 7 flows from the front gap 9 of the MR head, and this signal magnetic field is applied to the yoke. 8, the MR element 6, and the magnetic substrate 4. In the MR element 6, the resistance of the MR element changes in accordance with the strength of the signal magnetic field to perform electromagnetic conversion, and the lead layer performs the reading.
【0019】上記のような動作により、バルクハウゼン
ノイズは発生しない。これについてさらに詳しく説明す
る。Barkhausen noise is not generated by the above operation. This will be described in more detail.
【0020】図3はバイアス導体層5に印加する電流
と、MR素子6内の磁壁(磁化)の様子を示したもので
ある。図3において、(a)は導体層に印加する電流と
時間の関係、(b)〜(e)はMR素子6の磁壁(磁化
の向き)の模式図であり、E.Aは磁化容易軸を意味す
るもので、(a)の電流の印加する時間と対応付けて記
載されている。Y軸は記録媒体からの信号磁界の流入す
る方向である。本実施例においてはMR素子の磁化容易
軸はX軸に対し、+10度傾いている。FIG. 3 shows the current applied to the bias conductor layer 5 and the state of the domain wall (magnetization) in the MR element 6. 3, (a) is a relationship between the current applied to the conductor layer and time, (b) to (e) are schematic diagrams of the domain wall (magnetization direction) of the MR element 6, and FIG. A means the easy axis of magnetization, and is described in association with the time of applying the current in (a). The Y axis is the direction in which the signal magnetic field from the recording medium flows. In this embodiment, the easy axis of magnetization of the MR element is tilted +10 degrees with respect to the X axis.
【0021】まず、再生動作を行なう前では図3(b)
に示すようにMR素子6内には磁壁11が発生してい
る。First, before performing the reproducing operation, FIG.
As shown in FIG. 5, the domain wall 11 is generated in the MR element 6.
【0022】再生動作の開始とともに、バイアス導体層
5には直流電流I1 が印加され、これによる直流磁界
(Hbias1 )13により、MR素子内の磁化12はすべ
てY軸方向を向く(図3(c))。ここで、バイアス磁
界(Hbias1 )13はMR素子6の異方性磁界Hkより
大なる磁界強度である。A DC current I 1 is applied to the bias conductor layer 5 at the start of the reproducing operation, and a DC magnetic field (Hbias1) 13 generated by this causes all the magnetizations 12 in the MR element to face the Y-axis direction (see FIG. c)). The bias magnetic field (Hbias1) 13 has a magnetic field strength higher than the anisotropic magnetic field Hk of the MR element 6.
【0023】そして、バイアス導体層5に印加される直
流電流が電流がI2 まで連続的に減少する。このとき、
MR素子6内の磁化12は磁壁を発生することなく図3
(d)に示すように時計回りに回転するが、これはMR
素子6の磁化容易軸がX軸に対して傾いているため磁化
12と磁化容易軸との角度が時計回りの方向の方が小さ
いためで、もし、MR素子6の磁化容易軸がX軸に平行
であれば、異方性の分散等の要因により直流電流を減少
させたときにMR素子6内の磁化は時計回りに回転する
磁化成分14と反時計回りに回転する磁化成分15が生
じ、磁壁16を生じる(図3(f))。Then, the direct current applied to the bias conductor layer 5 continuously decreases until the current reaches I 2 . At this time,
The magnetization 12 in the MR element 6 does not generate a domain wall and
It rotates clockwise as shown in (d).
Since the easy axis of magnetization of the element 6 is inclined with respect to the X axis, the angle between the magnetization 12 and the easy axis of magnetization is smaller in the clockwise direction. If they are parallel, when the direct current is reduced due to factors such as anisotropic dispersion, the magnetization in the MR element 6 has a magnetization component 14 that rotates clockwise and a magnetization component 15 that rotates counterclockwise. The domain wall 16 is generated (FIG. 3 (f)).
【0024】バイアス導体層5に印加される電流がI2
になると、MR素子6内の磁化12はバイアス電流I2
から生じるバイアス磁界(Hbias2 )17により最適バ
イアス点を実現する方向を向く(図3(e))。The current applied to the bias conductor layer 5 is I 2
Then, the magnetization 12 in the MR element 6 becomes bias current I 2
The bias magnetic field (Hbias2) 17 generated from the magnetic field causes the optimum bias point to be realized (FIG. 3 (e)).
【0025】このような状態で、記録媒体7から信号磁
界がMR素子6内に流入すると、MR素子6内には磁壁
が存在しないためMR素子6の抵抗は連続的に変化しバ
ルクハウゼンノイズは発生せず、MR素子6の出力は良
好なものとなる。When the signal magnetic field from the recording medium 7 flows into the MR element 6 in such a state, the resistance of the MR element 6 continuously changes because there is no domain wall in the MR element 6, and Barkhausen noise is generated. It does not occur and the output of the MR element 6 becomes good.
【0026】本実施例において、MR素子6の磁化容易
軸の傾きを10度と設定したが、ノイズの抑制効果、再
生出力や、印加すべきバイアス電流I1 の大きさに鑑
み、容易軸の傾きを5〜30度であれば同様な効果を有
する。In the present embodiment, the inclination of the easy axis of the MR element 6 is set to 10 degrees, but in view of the noise suppressing effect, the reproduction output, and the magnitude of the bias current I 1 to be applied, the easy axis is set. If the inclination is 5 to 30 degrees, the same effect is obtained.
【0027】[0027]
【発明の効果】以上のように本発明による磁気記録再生
装置は、磁化容易軸が記録媒体からMRに流入する信号
磁束の流入方向の直角方向に対し5〜30度傾いたMR
素子とMR素子にバイアス磁界を印加する導体を有する
再生用薄膜磁気ヘッドと、バイアス磁界を印加する導体
に直流電流I1 を印加したのち連続的に電流値をI2
(I1>I2>0)に変化させる直流電流回路を有するこ
とにより、記録媒体を再生するときにMR素子内に磁壁
が発生していないためバルクハウゼンノイズのない良好
な再生出力を得ることができる。As described above, in the magnetic recording / reproducing apparatus according to the present invention, the MR axis having the easy axis of magnetization inclined by 5 to 30 degrees with respect to the direction perpendicular to the inflow direction of the signal magnetic flux flowing into the MR from the recording medium.
A thin film magnetic head for reproduction having a conductor for applying a bias magnetic field to the element and the MR element, and a direct current I 1 is applied to the conductor for applying a bias magnetic field, and then the current value is continuously changed to I 2.
By having a direct current circuit for changing to (I 1 > I 2 > 0), a magnetic domain wall is not generated in the MR element when reproducing the recording medium, so that a good reproduction output without Barkhausen noise can be obtained. You can
【図1】本発明の磁気記録再生装置の再生部ブロック図FIG. 1 is a block diagram of a reproducing section of a magnetic recording / reproducing apparatus of the present invention.
【図2】本発明の磁気記録再生装置の再生用MRヘッド
の断面図FIG. 2 is a sectional view of a reproducing MR head of a magnetic recording / reproducing apparatus of the present invention.
【図3】(a)は本発明の磁気記録再生装置のバイアス
電流の波形を表わす図 (b)はMR素子の磁壁(磁化)状態を表わす図 (c)はMR素子の磁壁(磁化)状態を表わす図 (d)はMR素子の磁壁(磁化)状態を表わす図 (e)はMR素子の磁壁(磁化)状態を表わす図 (f)はMR素子の磁壁(磁化)状態を表わす図3A is a diagram showing a waveform of a bias current of the magnetic recording / reproducing apparatus of the present invention, FIG. 3B is a diagram showing a domain wall (magnetization) state of the MR element, and FIG. 3C is a domain wall (magnetization) state of the MR element. (D) shows a domain wall (magnetization) state of the MR element (e) shows a domain wall (magnetization) state of the MR element (f) shows a domain wall (magnetization) state of the MR element
【図4】従来の磁気記録再生装置の再生用MRヘッドの
断面図FIG. 4 is a sectional view of a reproducing MR head of a conventional magnetic recording / reproducing apparatus.
【図5】磁壁の発生を表わす図FIG. 5 is a diagram showing generation of a domain wall.
1 MRヘッド 2 電流電源回路 3 再生回路 4、41 磁性基板 5、42 バイアス導体層 6、43 MR素子 7、44 記録媒体 8、45 ヨーク 9、46 前部ギャップ部 10、47 後部ギャップ部 11、16、48 磁壁 12、14、15 磁化 13、17 バイアス磁界 1 MR head 2 Current power supply circuit 3 Reproducing circuit 4, 41 Magnetic substrate 5, 42 Bias conductor layer 6, 43 MR element 7, 44 Recording medium 8, 45 Yoke 9, 46 Front gap part 10, 47 Rear gap part 11, 16, 48 Domain wall 12, 14, 15 Magnetization 13, 17 Bias magnetic field
Claims (1)
記磁気抵抗効果素子は記録媒体から前記磁気抵抗効果素
子に流入する信号磁束の流入方向の直角方向に対し5〜
30度傾いた磁化容易軸を持ち、前記磁気抵抗効果素子
にバイアス磁界を印加する導体を有する再生用薄膜磁気
ヘッドと、前記導体に電流値I1 を印加したのち連続的
に電流値をI2 (I1>I2>0)に減少させた直流電流
を印加する電流回路を具備することを特徴とする磁気記
録再生装置。1. A magnetoresistive effect element is used as an electromagnetic conversion element, and the magnetoresistive effect element is 5 to a direction perpendicular to an inflow direction of a signal magnetic flux flowing from the recording medium into the magnetoresistive effect element.
A reproducing thin-film magnetic head having a conductor that has an easy axis of magnetization inclined by 30 degrees and applies a bias magnetic field to the magnetoresistive effect element, and a current value I 1 is applied to the conductor, and then the current value is continuously changed to I 2 A magnetic recording / reproducing apparatus comprising a current circuit for applying a direct current reduced to (I 1 > I 2 > 0).
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP9278993A JPH06301934A (en) | 1993-04-20 | 1993-04-20 | Magnetic recording/reproducing apparatus |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP9278993A JPH06301934A (en) | 1993-04-20 | 1993-04-20 | Magnetic recording/reproducing apparatus |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH06301934A true JPH06301934A (en) | 1994-10-28 |
Family
ID=14064194
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP9278993A Pending JPH06301934A (en) | 1993-04-20 | 1993-04-20 | Magnetic recording/reproducing apparatus |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH06301934A (en) |
-
1993
- 1993-04-20 JP JP9278993A patent/JPH06301934A/en active Pending
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