JPH01224902A - Magnetic field impressing electromagnet for magneto-optical disk - Google Patents
Magnetic field impressing electromagnet for magneto-optical diskInfo
- Publication number
- JPH01224902A JPH01224902A JP5106988A JP5106988A JPH01224902A JP H01224902 A JPH01224902 A JP H01224902A JP 5106988 A JP5106988 A JP 5106988A JP 5106988 A JP5106988 A JP 5106988A JP H01224902 A JPH01224902 A JP H01224902A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic field
- parallel
- magneto
- optical disk
- coil group
- 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.)
- Granted
Links
- 230000035699 permeability Effects 0.000 claims abstract description 17
- 239000000696 magnetic material Substances 0.000 claims description 9
- 239000000126 substance Substances 0.000 abstract 2
- 238000010586 diagram Methods 0.000 description 8
- 238000000034 method Methods 0.000 description 7
- 238000001514 detection method Methods 0.000 description 4
- 230000000694 effects Effects 0.000 description 3
- 239000000758 substrate Substances 0.000 description 3
- 230000001678 irradiating effect Effects 0.000 description 2
- 230000005415 magnetization Effects 0.000 description 2
- 230000003287 optical effect Effects 0.000 description 2
- 229910002546 FeCo Inorganic materials 0.000 description 1
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical group [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 1
- 229910001030 Iron–nickel alloy Inorganic materials 0.000 description 1
- 230000003321 amplification Effects 0.000 description 1
- 239000004020 conductor Substances 0.000 description 1
- 238000001816 cooling Methods 0.000 description 1
- 238000012217 deletion Methods 0.000 description 1
- 230000037430 deletion Effects 0.000 description 1
- 230000004907 flux Effects 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 238000003199 nucleic acid amplification method Methods 0.000 description 1
- 230000002093 peripheral effect Effects 0.000 description 1
- 229910000889 permalloy Inorganic materials 0.000 description 1
- 239000004065 semiconductor Substances 0.000 description 1
- 229910000702 sendust Inorganic materials 0.000 description 1
- 229910000859 α-Fe Inorganic materials 0.000 description 1
Landscapes
- Recording Or Reproducing By Magnetic Means (AREA)
Abstract
Description
【発明の詳細な説明】 〔産業上の利用分野〕 本発明は光磁気ディスク用磁界印加電磁石に関する。[Detailed description of the invention] [Industrial application field] The present invention relates to a magnetic field applying electromagnet for a magneto-optical disk.
従来の光磁気記録において記録情報を消去する場合には
、外部磁界を記録時とは逆極性に印加し、レーザ光ビー
ムを記録時と同等の強度で記録媒体に一様に照射する、
いわゆる−括消去が行なわれている。即ち外部磁界印加
により記録媒体の磁化状態を記録前の初期状態に戻して
いる。When erasing recorded information in conventional magneto-optical recording, an external magnetic field is applied with the opposite polarity to that during recording, and a laser beam is uniformly irradiated onto the recording medium with the same intensity as during recording.
So-called -batch deletion is performed. That is, by applying an external magnetic field, the magnetization state of the recording medium is returned to the initial state before recording.
ここで、公知の外部磁界印加手段は、例えば空心コイル
を用いる方法、電磁石を用いる方法、あるいは永久磁石
を用いる方法がある。Here, known external magnetic field applying means include, for example, a method using an air-core coil, a method using an electromagnet, or a method using a permanent magnet.
前述の磁界印加手段において、記録時と消去時とでは通
常数100工ルステツド以上の印加磁界が必要であるた
めに、空心コイルを用いる場合には、コイルが大型化し
、これに伴って、磁界切換速度が遅くなるとともに、記
録媒体とコイルとの距離を充分に接近させないと所業の
印加磁界が得られないという欠点がある。また電磁石を
用いる場合にも、磁界印加手段は大型化し、コイルのイ
ンダクタンスが大きいために磁界切換速度が遅いという
欠点を生じている。さらに、永久磁石を用いる場合には
、機械的の駆動手段を用いて磁界を切換えるために複雑
な機構が必要であり、この場合も磁界切換速度は遅いも
のとなっている0以上述べたように、従来のいずれの外
部磁界印加手段によっても磁界切換速度は遅いために、
消去には前述の一括消去方式が用いられ、また記録する
時には、一定磁界印加中にレーザパワーを高速変調する
方法が用いられている。即ち、従来の装置では既に記録
された情報に新しい情報を高速で重ね書きするいわゆる
オーバーライド機能を持たせることが困難であるという
問題点がある。In the above-mentioned magnetic field applying means, an applied magnetic field of several hundred or more steps is usually required during recording and erasing, so when an air-core coil is used, the coil becomes large, and along with this, the magnetic field switching becomes difficult. This has the disadvantage that the speed is slow and that the desired applied magnetic field cannot be obtained unless the distance between the recording medium and the coil is sufficiently close. Further, when an electromagnet is used, the magnetic field applying means is large in size, and the magnetic field switching speed is slow due to the large inductance of the coil. Furthermore, when using permanent magnets, a complicated mechanism is required to switch the magnetic field using a mechanical drive means, and in this case as well, the magnetic field switching speed is slow. , since the magnetic field switching speed is slow with any conventional external magnetic field application means,
For erasing, the aforementioned batch erasing method is used, and for recording, a method is used in which laser power is modulated at high speed while a constant magnetic field is applied. That is, the conventional apparatus has a problem in that it is difficult to provide a so-called override function for rapidly overwriting new information on already recorded information.
本発明の目的は、このような従来の問題点を解決して、
大きい磁界の高速スイッチングを可能にする新規な外部
磁界印加手段を提供することにある。The purpose of the present invention is to solve such conventional problems,
The object of the present invention is to provide a novel means for applying an external magnetic field that enables high-speed switching of a large magnetic field.
本発明の光磁気ディスク用磁界印加電磁石は、光磁気デ
ィスクの片面に配置された高透磁率磁性帯体と、この高
透磁率磁性体の途中に設けられ、同一方向の磁界を発生
するn個のコイルが電気的に並列に接続された第1の並
列コイル群とこの第1の並列コイル群と逆方向の磁界を
発生するn個のコイルが電気的に並列に接続された第2
の並列コイル群とから構成し、この第1の並列コイル群
と第2の並列コイル群との一方の端子が接続されて全体
として3端子を有する電磁石と、この電磁石を光磁気デ
ィスクの面に対して垂直に移動させる圧電素子とを有す
ることにより構成される。The magnetic field applying electromagnet for a magneto-optical disk of the present invention includes a high magnetic permeability magnetic strip placed on one side of a magneto-optical disk, and n pieces of magnetic strip that are provided in the middle of this high permeability magnetic strip and generate a magnetic field in the same direction. a first parallel coil group in which n coils are electrically connected in parallel; and a second parallel coil group in which n coils that generate a magnetic field in the opposite direction to the first parallel coil group are electrically connected in parallel.
an electromagnet having three terminals as a whole by connecting one terminal of the first parallel coil group and the second parallel coil group; and an electromagnet that is connected to the surface of the magneto-optical disk. It is constructed by having a piezoelectric element that is moved perpendicularly to the piezoelectric element.
ここで高透磁率磁性体にはフェライト(MnZn、Ni
Znなど)、パーマロイ(NiFe)、センダスト、ア
モルファス(CoZr、CoZr、FeCoZr、Co
Nb、CoTa、CoHfなど)、鉄心などが考えられ
る。また、高透磁率磁性体の開磁路部は光磁気媒体を介
してレーザ集光用レンズと対向して設けられる。さらに
また第1及び第2のn個のコイルはそれぞれ電気的に並
列に接続され、第1及び第2のコイル群は一方の端子が
接続され、全体として3端子の電磁石を構成する。コイ
ルのインダクタンスは並列に接続されているために大幅
に減少する。従って、インダクタンスが小さいことによ
り、記録電流の立ち上がり時間が小さくなるので、磁界
の切換速度を大幅に早くすることができる。Here, the high permeability magnetic material is ferrite (MnZn, Ni
Zn, etc.), permalloy (NiFe), sendust, amorphous (CoZr, CoZr, FeCoZr, Co
Nb, CoTa, CoHf, etc.), iron core, etc. can be considered. Further, the open magnetic path portion of the high permeability magnetic material is provided to face the laser condensing lens via the magneto-optical medium. Furthermore, the first and second n coils are each electrically connected in parallel, and the first and second coil groups are connected at one terminal, thereby forming a three-terminal electromagnet as a whole. The inductance of the coils is significantly reduced due to their parallel connection. Therefore, since the inductance is small, the rise time of the recording current is shortened, so that the switching speed of the magnetic field can be significantly increased.
以下、本発明の実施例について図面を参照して説明する
。Embodiments of the present invention will be described below with reference to the drawings.
第1図は本発明の一実施例の構成図である0図において
光磁気ディスク用磁界印加電磁石は、光磁気ディスク基
板7の裏面に設けられた光磁気ディスク磁性膜8に面し
て開磁路を持った高透磁率磁性体1を設け、この高透磁
率磁性体1の途中に電気的に並列に接続された第1の並
列コイル群2と第2のコイル群3とを設け、この第1の
並列コイル群と第2の並列コイル群とは一方の端子が接
続されて構成されている。記録電流は第1の並列コイル
と第2の並列コイルとに交互に電磁石駆動回路4から供
給される。また高透磁率磁性体1は圧電素子5によって
支持され、圧電素子5は圧電素子駆動回路6によって駆
動され、圧電素子5を駆動することによって、常時、光
磁気ディスク磁性膜面に間隙lを保って支持されている
高透磁率磁性体1を光磁気ディスク磁性膜面から引離し
て、光磁気ディスクの着脱を容易にすることができる。FIG. 1 is a configuration diagram of an embodiment of the present invention. In FIG. A high magnetic permeability magnetic body 1 having a path is provided, and a first parallel coil group 2 and a second coil group 3 electrically connected in parallel are provided in the middle of this high magnetic permeability magnetic body 1. The first parallel coil group and the second parallel coil group are configured with one terminal connected to each other. Recording current is alternately supplied from the electromagnet drive circuit 4 to the first parallel coil and the second parallel coil. The high permeability magnetic material 1 is supported by a piezoelectric element 5, which is driven by a piezoelectric element drive circuit 6. By driving the piezoelectric element 5, a gap l is always maintained between the magnetic film surface of the magneto-optical disk. The high magnetic permeability magnetic body 1 supported by the magneto-optical disk can be separated from the magnetic film surface of the magneto-optical disk to facilitate attachment and detachment of the magneto-optical disk.
第2図は第1図の回路図で、それぞれ複数本の絶縁導体
によって作られた第1の並列コイル群2と第2の並列コ
イル群3と、これらの並列コイル群を駆動する電磁石駆
動回路4とが示されている。電磁石駆動回路4から第1
および第2の並列コイル群2.3へ交互に電流を流すこ
とによって、記録媒体に垂直成分の印加磁界が与えられ
る。また高透磁率磁性体1は厚さ31m1、磁気量路長
(ギャップ、)約う龍のものが用いられ、また第1と第
2のコイル群としては、線径150μmのものをもちい
た。また電流値として数10mA〜1.OAが適当であ
る。このようにして構成した磁界印加手段では、コイル
を電気的に並列に接続しているためにコイルのインダク
タンスLを1μH以下にすることが容易なため、高透磁
率磁性体の端面から数龍離れた位置において、数100
エルステツドの磁界を数MHzの高速で容易に切換える
ことができる。Figure 2 is a circuit diagram of Figure 1, showing a first parallel coil group 2 and a second parallel coil group 3, each made of a plurality of insulated conductors, and an electromagnet drive circuit that drives these parallel coil groups. 4 is shown. From the electromagnet drive circuit 4 to the first
By alternately passing current through the second parallel coil group 2.3, an applied magnetic field with a perpendicular component is applied to the recording medium. The high permeability magnetic material 1 was made of a material having a thickness of 31 m1 and a magnetic path length (gap) of approximately 1.5 m, and the first and second coil groups used had wire diameters of 150 .mu.m. In addition, the current value ranges from several tens of mA to 1. OA is appropriate. In the magnetic field applying means configured in this way, since the coils are electrically connected in parallel, it is easy to reduce the inductance L of the coil to 1 μH or less. At the position, several hundred
The Oersted magnetic field can be easily switched at a high speed of several MHz.
第3図は第1図の実施例に周辺系を付加した光磁気記録
再生装置の構成図で、この装置により、光磁気ディスク
への記録再生消去を行なった。第3図において電磁石駆
動回路4の出力電流が第1の並列コイル群2および第2
の並列コイル群3に流れ、光磁気ディスク磁性膜2で構
成された記録媒体に上向き及び下向きの磁界が交互に印
加される。FIG. 3 is a block diagram of a magneto-optical recording and reproducing apparatus in which a peripheral system is added to the embodiment shown in FIG. 1. This apparatus was used to perform recording, reproduction and erasure on a magneto-optical disk. In FIG. 3, the output current of the electromagnet drive circuit 4 is
upward and downward magnetic fields are alternately applied to the recording medium constituted by the magneto-optical disk magnetic film 2.
光磁気記録用ヘッド31は従来と同等のものであり、次
のような構成を有する。32は直線偏光のレーザ光源で
あり、例えば半導体レーザが使用される。33,34.
35はビームスプリッタである。レーザ光ビーム集光用
レンズ36はアクチュエータ37により支持されている
。フォーカスエラーおよびトラッキングエラー信号はそ
れぞれフォーカスエラー信号検出用受光素子38.トラ
ッキングエラー信号検出用受光素子39によってサーボ
制御回路40.41に入力され、サーボ信号となり、ア
クチュエータ37にフィードバックされる。再生信号は
偏光フィルタ42を通過後、再生信号用受光素子43に
よって検出され、再生信号増幅回路44によって増幅さ
れる。偏光フィルタ42としてはダラムトムソンプリズ
ムを用い、再生信号検出用受光素子43としてはPIN
フォトダイオードを用いた。レーザ光源32の変調には
レーザ光源変調回路45が使用され、記録時、消去時、
再生時に合わせてレーザ光のパワーが変調される。The magneto-optical recording head 31 is the same as the conventional one, and has the following configuration. 32 is a linearly polarized laser light source, for example, a semiconductor laser is used. 33, 34.
35 is a beam splitter. The laser beam focusing lens 36 is supported by an actuator 37. The focus error signal and the tracking error signal are detected by the focus error signal detection light receiving element 38. The tracking error signal detection light receiving element 39 inputs the tracking error signal to the servo control circuit 40 , 41 , becomes a servo signal, and feeds it back to the actuator 37 . After passing through the polarizing filter 42 , the reproduced signal is detected by the reproduced signal light receiving element 43 and amplified by the reproduced signal amplification circuit 44 . A Durham Thomson prism is used as the polarizing filter 42, and a PIN is used as the light receiving element 43 for detecting the reproduced signal.
A photodiode was used. A laser light source modulation circuit 45 is used to modulate the laser light source 32, and when recording, erasing,
The power of the laser beam is modulated in accordance with the reproduction time.
光磁気ディスクとして1201径のプラスチック基板上
にスパッタ法により形成されたSiN上に、さらにTb
FeCo膜を800オングストローム厚に、形成し、こ
のTbFeCo膜上にSiNを形成したディスクを使用
した。基板としては予めトラックピッチ1.6μm、深
さ700オングストロームの溝が形成されたいわゆるプ
リグループ基板を用いた。As a magneto-optical disk, Tb
A disk was used in which a FeCo film was formed to a thickness of 800 angstroms and SiN was formed on the TbFeCo film. The substrate used was a so-called pre-group substrate in which grooves with a track pitch of 1.6 μm and a depth of 700 angstroms were formed in advance.
第4図(a)〜(C)は記録の動作モード図である。記
録媒体をキュリー温度以上に上昇できる一定強度のレー
ザビームを照射しながら、外部磁界印加のための第1と
第2との並列コイル群2゜3に第4図(b)に示すよう
な変調電流を流すことによって、記録パターンに対応し
た外部磁界が印加され、記録媒体の走行に伴なう冷却過
程で印加磁界方向に対応して、第4図(C)に示すよう
な記録磁化状態が実現される。まず線速9m/secに
てディスク面上10mWの一定強度レーザ光を照射しな
がら、外部磁界印加手段のコイル2.3にIMHzで、
200mAの変調電流を流したところ、良好な記録がで
きた。この記録トラック上に新たに同一条件で記録磁界
を0.5MHzで印加したところ、この記録磁界に対応
した記録ができ、前に記録した信号の消え残りは28d
Bであり、十分実用性があることが分かった。FIGS. 4(a) to 4(C) are recording operation mode diagrams. While irradiating a laser beam with a constant intensity that can raise the recording medium above the Curie temperature, modulation as shown in Figure 4(b) is applied to the first and second parallel coil groups 2°3 for applying an external magnetic field. By passing a current, an external magnetic field corresponding to the recording pattern is applied, and during the cooling process as the recording medium runs, the recording magnetization state as shown in FIG. 4(C) is changed according to the direction of the applied magnetic field. Realized. First, while irradiating a constant intensity laser beam of 10 mW onto the disk surface at a linear velocity of 9 m/sec, the coil 2.3 of the external magnetic field applying means was applied with IMHz.
Good recording was achieved when a modulation current of 200 mA was applied. When a recording magnetic field of 0.5 MHz was newly applied to this recording track under the same conditions, recording corresponding to this recording magnetic field was achieved, and the previously recorded signal remained for 28 d.
B, and it was found to be sufficiently practical.
以上述べたように本発明によれば、光磁気ディスクの片
面に複数本の並列コイルを有する一体の高透磁率磁性体
を用いているので、コイルのインダクタンスを小さくで
き、大きい磁界の高速スイッチングが可能であり、且つ
磁束利用効率の良い光磁気ディスク用磁界印加電磁石を
提供できる。As described above, according to the present invention, since an integrated high permeability magnetic material having multiple parallel coils is used on one side of the magneto-optical disk, the inductance of the coil can be reduced and high-speed switching of large magnetic fields can be achieved. It is possible to provide a magnetic field applying electromagnet for a magneto-optical disk that is possible and has high magnetic flux utilization efficiency.
従って、光磁気記録再生方式では従来の一括消去を必要
とせずに直接所望の記録が可能なオーバーライド性能が
実現できるという効果がある。また光磁気ディスクの片
面にのみ高透磁率磁性体が設けられているので、圧電素
子を用いて高透磁率磁性体を移動できるので、光磁気デ
ィスクの取扱いが容易にできる効果がある。Therefore, the magneto-optical recording and reproducing method has the effect of realizing override performance that allows desired recording to be performed directly without requiring the conventional batch erasing. Furthermore, since the high permeability magnetic material is provided only on one side of the magneto-optical disk, the high permeability magnetic material can be moved using a piezoelectric element, which has the effect of making it easier to handle the magneto-optical disk.
第1図は本発明の一実施例の構成図、第2図は第1図の
回路図、第3図は第1図の実施例を光磁気ディスク装置
に適用した場合の構成図、第4図は第3図の記録の動作
モード図である。
1・・・高透磁率磁性体、2・・・第1の並列コイル群
、3・・・第2の並列コイル群、4・・・電磁石駆動回
路、5・・・圧電素子、6・・・圧電素子駆動回路、1
1・・・光デイスク基板、12・・・光デイスク磁性媒
体、31・・・光磁気記録用ヘッド、32・・・レーザ
光源、33.34.35・・・ビームスプリッタ、36
・・・レーザ光ビーム集光レンズ、37・・・アクチュ
エータ、38・・・フォーカスエラー信号検出用受光素
子、39・・・トラッキング信号検出用受光素子、40
.41・・・サーボ制御回路、42・・・偏光フィルタ
、43・・・再生信号検出用受光素子、44・・・増幅
回路、45・・・レーザ光源変調回路。1 is a configuration diagram of an embodiment of the present invention, FIG. 2 is a circuit diagram of FIG. 1, FIG. 3 is a configuration diagram of the embodiment of FIG. 1 applied to a magneto-optical disk device, and FIG. The figure is an operational mode diagram of the recording of FIG. 3. DESCRIPTION OF SYMBOLS 1... High permeability magnetic material, 2... First parallel coil group, 3... Second parallel coil group, 4... Electromagnet drive circuit, 5... Piezoelectric element, 6...・Piezoelectric element drive circuit, 1
DESCRIPTION OF SYMBOLS 1... Optical disk substrate, 12... Optical disk magnetic medium, 31... Magneto-optical recording head, 32... Laser light source, 33.34.35... Beam splitter, 36
... Laser light beam condensing lens, 37... Actuator, 38... Light receiving element for focus error signal detection, 39... Light receiving element for tracking signal detection, 40
.. 41... Servo control circuit, 42... Polarizing filter, 43... Light receiving element for detecting reproduced signal, 44... Amplifying circuit, 45... Laser light source modulation circuit.
Claims (1)
、この高透磁率磁性体の途中に設けられ、同一方向の磁
界を発生するn個のコイルが電気的に並列に接続された
第1の並列コイル群とこの第1の並列コイル群と逆方向
の磁界を発生するn個のコイルが電気的に並列に接続さ
れた第2の並列コイル群とから構成し、この第1の並列
コイル群と第2の並列コイル群との一方の端子が接続さ
れて全体として3端子を有する電磁石と、この電磁石を
光磁気ディスクの面に対して垂直に移動させる圧電素子
とを有することを特徴とする光磁気ディスク用磁界印加
電磁石。A high permeability magnetic strip placed on one side of the magneto-optical disk and n coils installed in the middle of this high permeability magnetic material and generating magnetic fields in the same direction are electrically connected in parallel. The first parallel coil group consists of one parallel coil group and a second parallel coil group in which n coils that generate a magnetic field in the opposite direction to the first parallel coil group are electrically connected in parallel. It is characterized by having an electromagnet that has three terminals as a whole by connecting one terminal of the coil group and the second parallel coil group, and a piezoelectric element that moves this electromagnet perpendicularly to the surface of the magneto-optical disk. Magnetic field applying electromagnet for magneto-optical disks.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP5106988A JP2811673B2 (en) | 1988-03-03 | 1988-03-03 | Magnetic field applying electromagnet for magneto-optical disk |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP5106988A JP2811673B2 (en) | 1988-03-03 | 1988-03-03 | Magnetic field applying electromagnet for magneto-optical disk |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH01224902A true JPH01224902A (en) | 1989-09-07 |
JP2811673B2 JP2811673B2 (en) | 1998-10-15 |
Family
ID=12876515
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP5106988A Expired - Fee Related JP2811673B2 (en) | 1988-03-03 | 1988-03-03 | Magnetic field applying electromagnet for magneto-optical disk |
Country Status (1)
Country | Link |
---|---|
JP (1) | JP2811673B2 (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH04103322U (en) * | 1991-01-28 | 1992-09-07 | テイアツク株式会社 | magnetic head device |
EP0559469A2 (en) * | 1992-03-06 | 1993-09-08 | Canon Kabushiki Kaisha | Magnetic head driving device and magnetooptical recording apparatus |
EP0622792A2 (en) * | 1993-03-26 | 1994-11-02 | Canon Kabushiki Kaisha | Magnetic head driving apparatus and magnetooptical recording apparatus |
-
1988
- 1988-03-03 JP JP5106988A patent/JP2811673B2/en not_active Expired - Fee Related
Cited By (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH04103322U (en) * | 1991-01-28 | 1992-09-07 | テイアツク株式会社 | magnetic head device |
EP0559469A2 (en) * | 1992-03-06 | 1993-09-08 | Canon Kabushiki Kaisha | Magnetic head driving device and magnetooptical recording apparatus |
EP0559469A3 (en) * | 1992-03-06 | 1994-02-16 | Canon Kk | |
EP0622792A2 (en) * | 1993-03-26 | 1994-11-02 | Canon Kabushiki Kaisha | Magnetic head driving apparatus and magnetooptical recording apparatus |
EP0622792A3 (en) * | 1993-03-26 | 1994-12-14 | Canon Kk | Magnetic head driving apparatus and magnetooptical recording apparatus. |
Also Published As
Publication number | Publication date |
---|---|
JP2811673B2 (en) | 1998-10-15 |
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Legal Events
Date | Code | Title | Description |
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LAPS | Cancellation because of no payment of annual fees |