JPH01178105A - Magnetic field electromagnet for magneto-optical disk - Google Patents
Magnetic field electromagnet for magneto-optical diskInfo
- Publication number
- JPH01178105A JPH01178105A JP95388A JP95388A JPH01178105A JP H01178105 A JPH01178105 A JP H01178105A JP 95388 A JP95388 A JP 95388A JP 95388 A JP95388 A JP 95388A JP H01178105 A JPH01178105 A JP H01178105A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic field
- magneto
- high permeability
- optical disk
- permeability 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.)
- Granted
Links
- 230000035699 permeability Effects 0.000 claims abstract description 33
- 238000000926 separation method Methods 0.000 claims abstract description 9
- 239000000696 magnetic material Substances 0.000 claims description 15
- 230000007246 mechanism Effects 0.000 claims description 6
- 239000000126 substance Substances 0.000 abstract 10
- 238000000034 method Methods 0.000 description 8
- 238000010586 diagram Methods 0.000 description 6
- 239000000758 substrate Substances 0.000 description 4
- 238000001514 detection method Methods 0.000 description 3
- 230000003287 optical effect Effects 0.000 description 3
- 239000010409 thin film Substances 0.000 description 3
- 230000003321 amplification Effects 0.000 description 2
- 239000010408 film Substances 0.000 description 2
- 230000001678 irradiating effect Effects 0.000 description 2
- 230000005415 magnetization Effects 0.000 description 2
- 238000003199 nucleic acid amplification method Methods 0.000 description 2
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical group [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 1
- 229910001030 Iron–nickel alloy Inorganic materials 0.000 description 1
- 229910003962 NiZn Inorganic materials 0.000 description 1
- 230000008901 benefit Effects 0.000 description 1
- 230000008859 change Effects 0.000 description 1
- 239000003795 chemical substances by application Substances 0.000 description 1
- 238000001816 cooling Methods 0.000 description 1
- 230000008878 coupling Effects 0.000 description 1
- 238000010168 coupling process Methods 0.000 description 1
- 238000005859 coupling reaction Methods 0.000 description 1
- 238000012217 deletion Methods 0.000 description 1
- 230000037430 deletion Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- -1 etc.) Inorganic materials 0.000 description 1
- 230000004907 flux Effects 0.000 description 1
- 230000002093 peripheral effect Effects 0.000 description 1
- 229910000889 permalloy Inorganic materials 0.000 description 1
- 230000008569 process Effects 0.000 description 1
- 239000004065 semiconductor Substances 0.000 description 1
- 229910000702 sendust Inorganic materials 0.000 description 1
- 238000004544 sputter deposition Methods 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
、外部磁界製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
によシ記録媒体の磁化状態は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要の
印加磁界が得られないという欠点がある。また電磁石音
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
、機械的な駆動手段を用いて磁界を切シ変えるために複
雑壜機構が必要であシ、この場合も磁界切換速度は遅い
ものとなっている。以上の述べたように、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
するときには、一定磁界印加中にレーザノくワーを高速
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 method has the disadvantage that the speed is slow and that the required applied magnetic field cannot be obtained unless the distance between the recording medium and the coil is sufficiently close. Furthermore, when electromagnetic sound is used, the magnetic field applying means is large in size and the inductance of the coil is large, resulting in a slow magnetic field switching speed. Furthermore, when permanent magnets are used, a complicated bottle mechanism is required to switch the magnetic field using mechanical drive means, and the switching speed of the magnetic field is also slow in this case. As mentioned above, the magnetic field switching speed is slow with any conventional external magnetic field applying means, so the aforementioned batch erasing method is used for erasing, and when recording, the laser beam is turned off while a constant magnetic field is applied. A method of high-speed modulation is used. 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
磁界印加手段を有して、さらに光ディスクの脱着を容易
にする光磁気ディスク用磁界印加電磁石を提供すること
にある。The purpose of the present invention is to solve such conventional problems,
It is an object of the present invention to provide a magnetic field applying electromagnet for a magneto-optical disk, which has a novel external magnetic field applying means that enables high-speed switching of a large magnetic field, and further facilitates the attachment and detachment of an optical disk.
〔問題点を解決する為の手段〕
本発明の光磁気ディスク用磁界印加電磁石は、光磁気デ
ィスクの周辺部で折返してU字形とし、この折返し部分
に分離境界を有し、このU字形の二つの直線部が前記光
磁気ティスフの両面のそれぞれに対面した高透磁率磁性
体と、前記直線部の一つの一端に設けられた中空部のま
わりの光磁気ディスクの面側に設けた第1のコイルと、
前記直線部の少なくとも一方に前記第1のコイルと同一
方向の磁界を発生するように設けられた複数のコイルと
、前記U字形の高透磁率磁性体を前記分離境界で分離・
結合する接続機構とを有して構成される。[Means for Solving the Problems] The magnetic field applying electromagnet for a magneto-optical disk of the present invention is folded around the periphery of the magneto-optical disk to form a U-shape, has a separation boundary at this folded portion, and has a separation boundary between the two sides of the U-shape. A high magnetic permeability magnetic material having two linear portions facing each of both sides of the magneto-optical disk, and a first magnetic material provided on the surface side of the magneto-optical disk around a hollow portion provided at one end of one of the linear portions. coil and
A plurality of coils provided in at least one of the straight portions to generate a magnetic field in the same direction as the first coil and the U-shaped high permeability magnetic body are separated at the separation boundary.
and a connecting mechanism for coupling.
ここで高透磁率磁性体にはフェライ) (MnZn。Here, the high permeability magnetic material is ferrite) (MnZn.
NiZnなど)、パーマロイ(NiFe)、センダスト
、7−F−A/7 ア、x、(CoZr 、FeCoZ
r 、CoNb。NiZn, etc.), Permalloy (NiFe), Sendust, 7-F-A/7 a, x, (CoZr, FeCoZ
r, CoNb.
CoTa、CoHfなど)、鉄心などが考えられる。(CoTa, CoHf, etc.), iron core, etc.
また、同心円状の中空を有するU字形の高透磁率磁性体
はレーザ集光用レンズと光磁気媒体の間に設定し、その
中空の内径はレーザビームが通過でき、かつトラッキン
ダによりトラツタ方向にレンズが動かせる程度の大きさ
に設定される。In addition, a U-shaped high magnetic permeability magnetic body with a concentric hollow is set between the laser condensing lens and the magneto-optical medium, and the inner diameter of the hollow allows the laser beam to pass through, and the tracker moves the lens in the track direction. The size is set so that it can be moved.
また、U字型高透磁率磁性体の上半分はもう一つの電磁
石によって分離できるようにして、光磁気ディスクの脱
着が容易に出来るようにする。従って光磁気ディスクが
セットされているときは、U字型高透磁率磁性体の二つ
の直線部は磁気的に結合し、光磁気ディスクが取り外さ
れているときはU字型高透磁率磁性体の二つの直線部は
磁気的に分離される。このようにすることによシ、光磁
気ディスクの脱着を容易にし、且つオーツ(−ライトに
十分な磁界を高速で発生する。Further, the upper half of the U-shaped high permeability magnetic body can be separated by another electromagnet, so that the magneto-optical disk can be easily attached and detached. Therefore, when the magneto-optical disk is set, the two straight parts of the U-shaped high permeability magnetic material are magnetically coupled, and when the magneto-optical disk is removed, the U-shaped high permeability magnetic material is magnetically coupled. The two straight sections are magnetically separated. By doing so, the magneto-optical disk can be easily attached and detached, and a magnetic field sufficient for writing can be generated at high speed.
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。この実施例
では光磁気ディスク11の周辺部で折返してU字形とし
た高透磁率磁性体が、この折返し部分に分離境界面を持
った第1の高透磁率磁性体1と第2の高透磁率磁性体2
とによシ形成され、第1および第2の高透磁率磁性体1
および2はそれぞれ光磁気ディスク11の表面および裏
面に対面している。さらに第1の高透磁率磁性体lの先
端に設けられた中空部21のまわシの光磁気ディスク面
側に第1のコイル8が設けられ、第2の高透磁率磁性体
2には磁界発生電流変調回路10からの記録電流により
、第1のコイル8に発生する磁界の方向と同じ方向に磁
界が発生するコイル7および9が設けられている。さら
にまた固定された第2の高透磁率磁性体2から第1の高
透磁率磁性体lを分離・結合するための磁石分離機構3
が設けられた構成となっている。FIG. 1 is a block diagram of an embodiment of the present invention. In this embodiment, a high permeability magnetic material is folded in a U-shape at the periphery of the magneto-optical disk 11, and a first high permeability magnetic material 1 and a second high permeability magnetic material 1, each having a separating boundary surface at the folded portion, are formed into a U-shaped high permeability magnetic material. Magnetic property magnetic material 2
first and second high permeability magnetic bodies 1
and 2 face the front and back surfaces of the magneto-optical disk 11, respectively. Further, a first coil 8 is provided on the magneto-optical disk surface side of the hollow portion 21 provided at the tip of the first high permeability magnetic body 1, and a magnetic field is applied to the second high permeability magnetic body 2. Coils 7 and 9 are provided in which a magnetic field is generated in the same direction as the magnetic field generated in the first coil 8 by the recording current from the generated current modulation circuit 10. Furthermore, a magnet separation mechanism 3 for separating and combining the first high magnetic permeability magnetic body l from the fixed second high magnetic permeability magnetic body 2
The structure is set up.
以上の構成において磁界発生電流変調回路10からコイ
ル7.8および9に電流を流すことにより、光磁気ディ
スク11の裏面側に設けられた磁性薄膜12である記録
媒体に垂直方向の印加磁界が与えられる。なお、第1お
よび第2の高透磁率磁性体11の合計長は約20cmの
ものが用いられ、コイル7.8および9の線径は150
μm程度、電流値としては10mA〜1.OAが適当で
ある。In the above configuration, by flowing current from the magnetic field generation current modulation circuit 10 to the coils 7.8 and 9, a perpendicular magnetic field is applied to the recording medium, which is the magnetic thin film 12 provided on the back side of the magneto-optical disk 11. It will be done. Note that the total length of the first and second high permeability magnetic bodies 11 is about 20 cm, and the wire diameter of the coils 7.8 and 9 is 150 cm.
about μm, and the current value is 10 mA to 1. OA is appropriate.
このようにして構成した磁界印加手段では、コイルのイ
ンダクタンスLを、小さくすることが容易なため、高透
磁率磁性体の端面から数mm離れた位置において、数1
00エルステ、ドの磁界を数MHzの高速で容易に切シ
変ることができる。With the magnetic field applying means configured in this manner, it is easy to reduce the inductance L of the coil, so that it is easy to reduce the inductance L of the coil, so that the inductance L of the coil can be easily reduced by
It is possible to easily change the magnetic field of 00 oerste or de at a high speed of several MHz.
第2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
11への記録再生消去を行なった。FIG. 2 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.
第2図において磁界発生電流変調回路lOの出力電流が
コイル7.8および9に流れ、光磁気ディスク11の磁
性薄膜12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。In FIG. 2, the output current of the magnetic field generation current modulation circuit 10 flows through coils 7.8 and 9, and upward and downward magnetic fields are alternately applied to the recording medium composed of the magnetic thin film 12 of the magneto-optical disk 11.
光磁気記録用へ、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
あシ、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、りである。レーザ光ビーム集光用
レンズ36はアクチエエータ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
、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、サーボ信号となシ、ア
クチュエータ37にフィードパ、りされる。再生信号は
偏光フィルタ42t−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としてはグラムトムンンプリ
ズムを用い、再生信号検出用受光素子43としてはPI
N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 card 31 for magneto-optical recording 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 signal is input to the servo control circuit 40, 41 by the light receiving element 39 for detecting the error signal, and is fed to the actuator 37 as a servo signal. After the reproduced signal passes through the polarizing filter 42t, it passes through the reproduced signal light receiving element 43.
and is amplified by the reproduction signal amplification circuit 44. A Gram-Tommon prism is used as the polarizing filter 42, and a PI is used as the light receiving element 43 for detecting the reproduced signal.
An N photodiode was used. A laser light source modulation circuit 45 is used to modulate the laser light source 32, and the power of the laser light is modulated during recording, erasing, and reproduction.
光磁気ディスクとして120mm径のプラスチ、り基板
上にスバ、り法により形成されたSiN上に、さらにT
b F e Co膜を800オングストローム厚に、
形成し、このTbFeCo膜上にさらに5iNt?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, T was further deposited on SiN formed on a plastic substrate with a diameter of 120 mm by a sputtering method.
b F e Co film with a thickness of 800 angstroms,
5iNt? is further formed on this TbFeCo film. The formed disc was used. 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3図(a)〜(C)は記録の動作モード図である。記
録媒体t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コイル
7.8および9に第3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3図(C)に示すような記録磁化状
態が実現される。3(a) to 3(C) are recording operation mode diagrams. Recording is performed by passing a modulated current as shown in FIG. 3(b) through the coils 7.8 and 9 for applying an external magnetic field while irradiating a laser beam with a constant intensity that can raise the temperature above the Curie temperature of the recording medium. An external magnetic field corresponding to the pattern is applied, and a recording magnetization state as shown in FIG. 3(C) is realized in accordance with the direction of the applied magnetic field during the cooling process accompanying the running of the recording medium.
まず線速9m/secにてディスク面上4mW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
7.8および9にIMHzで、800mAの変調電流會
流したところ、良好な記録かで 4きた。この記録トラ
、り上に新たに同一条件で記録磁界’k 0.5 M
Hz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シはみられなかった。First, while irradiating a laser beam with a constant intensity of 4 mW onto the disk surface at a linear velocity of 9 m/sec, a modulated current of 800 mA at IMHz was applied to coils 7.8 and 9 of the external magnetic field applying means. So it's 4. On this recording track, a new recording magnetic field 'k 0.5 M is applied under the same conditions.
When applied at Hz, recording corresponding to this recording magnetic field was possible, and no trace of previously recorded signals remained.
以上述べたように本発明によれば、光磁気ディスクの両
側に対面する高透磁率磁性体には二つに分離できる高透
磁率磁性体を用い、且つとの高透磁率磁性体の上半分と
固定された下半分とを分離・結合できる機構を有してい
るために光ディスクの脱着が容易であり、さらにコイル
のインダクタンスを小さくできるために大きい磁界の高
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, a high permeability magnetic material that can be separated into two is used as the high permeability magnetic material facing both sides of the magneto-optical disk, and the upper half of the high permeability magnetic material is separated into two parts. Because it has a mechanism that can separate and connect the fixed lower half, it is easy to attach and detach the optical disk.Furthermore, since the inductance of the coil can be reduced, high-speed switching of a large magnetic field is possible, and it is possible to utilize magnetic flux. It is possible to provide an efficient magnetic field applying electromagnet for a magneto-optical disk.
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、且つディスクの脱着が容易になるという効果
がある。Therefore, the magneto-optical recording and reproducing method has the advantage that it is possible to achieve override performance that allows desired recording to be performed directly without the need for conventional batch erasing, and that the disk can be easily attached and detached.
第1図は本発明の一実施例の構成図、第2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3図は第2図の記録の動作モード図である。
1.2・・・・・・高透磁率磁性体、3・・・・・・磁
石分離機構、7,8,9・・・・・・コイル、10・・
・・・・磁界発生電流変調発生回路、21・・・・・・
中空部、31・・・・・・光磁気記録用へ、ド、11・
・・・・・光デイスク基板、12・・・・・・磁性薄膜
、32・・・・・・レーザ光源、33,34゜15・・
・・・・ビームスプリ、り、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、キングエラー信号検出用受光
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。
代理人 弁理士 内 原 音
芽 3 図FIG. 1 is a block diagram of an embodiment of the present invention, FIG. 2 is a block diagram of the embodiment of FIG. 1 applied to a magneto-optical disk device,
FIG. 3 is an operational mode diagram of the recording shown in FIG. 2. 1.2... High permeability magnetic material, 3... Magnet separation mechanism, 7, 8, 9... Coil, 10...
...Magnetic field generation current modulation generation circuit, 21...
Hollow part, 31...For magneto-optical recording, C, 11.
...Optical disk substrate, 12...Magnetic thin film, 32...Laser light source, 33, 34°15...
・・・Beam splitter, 36...Laser light beam condensing lens, 37...Actuator,
38... Light receiving element for focus error signal detection, 39... Light receiving element for king error signal detection, 40° 41... Servo control circuit, 42...
... Polarizing filter, 43 ... Light receiving element for detecting reproduced signal, 44 ... Amplification circuit, 45 ...
...Laser light source modulation circuit. Agent Patent Attorney Otome Uchihara 3 Figure
Claims (1)
返し部分に分離境界を有し、このU字形の二つの直線部
が前記光磁気ディスクの両面のそれぞれに対面した高透
磁率磁性体と、前記直線部の一つの一端に設けられた中
空部のまわりの光磁気ディスクの面側に設けた第1のコ
イルと、前記直線部の少なくとも一方に前記第1のコイ
ルと同一方向の磁界を発生するように設けられた複数の
コイルと、前記U字形の高透磁率磁性体を前記分離境界
で分離・結合する接続機構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 magnetic permeability magnetic material that is folded back at the periphery of the magneto-optical disk to form a U-shape, has a separation boundary at the folded portion, and two straight portions of the U-shape face each of both surfaces of the magneto-optical disk; A first coil provided on the surface side of the magneto-optical disk around a hollow portion provided at one end of one of the linear portions generates a magnetic field in the same direction as the first coil in at least one of the linear portions. 1. A magnetic field applying electromagnet for a magneto-optical disk, comprising: a plurality of coils arranged to do so; and a connection mechanism that separates and connects the U-shaped high permeability magnetic body at the separation boundary.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP95388A JPH067401B2 (en) | 1988-01-05 | 1988-01-05 | Magnetic field applying electromagnet for magneto-optical disk |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP95388A JPH067401B2 (en) | 1988-01-05 | 1988-01-05 | Magnetic field applying electromagnet for magneto-optical disk |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH01178105A true JPH01178105A (en) | 1989-07-14 |
| JPH067401B2 JPH067401B2 (en) | 1994-01-26 |
Family
ID=11488038
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP95388A Expired - Fee Related JPH067401B2 (en) | 1988-01-05 | 1988-01-05 | Magnetic field applying electromagnet for magneto-optical disk |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH067401B2 (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH04283436A (en) * | 1991-03-11 | 1992-10-08 | Sharp Corp | Magneto-optical disk device |
-
1988
- 1988-01-05 JP JP95388A patent/JPH067401B2/en not_active Expired - Fee Related
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH04283436A (en) * | 1991-03-11 | 1992-10-08 | Sharp Corp | Magneto-optical disk device |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH067401B2 (en) | 1994-01-26 |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| LAPS | Cancellation because of no payment of annual fees |