JPH08227542A - Magneto-optical recording and reproducing device - Google Patents

Magneto-optical recording and reproducing device

Info

Publication number
JPH08227542A
JPH08227542A JP30528795A JP30528795A JPH08227542A JP H08227542 A JPH08227542 A JP H08227542A JP 30528795 A JP30528795 A JP 30528795A JP 30528795 A JP30528795 A JP 30528795A JP H08227542 A JPH08227542 A JP H08227542A
Authority
JP
Japan
Prior art keywords
recording
magnetic field
light
information
magneto
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
Application number
JP30528795A
Other languages
Japanese (ja)
Other versions
JP2744776B2 (en
Inventor
Kenji Ota
賢司 太田
Toshihisa Deguchi
敏久 出口
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.)
Sharp Corp
Original Assignee
Sharp Corp
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
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Priority to JP7305287A priority Critical patent/JP2744776B2/en
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Application granted granted Critical
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Links

Abstract

PURPOSE: To suppress the generation of heat and to control the magnetic field generated from an electromagnet at a high speed by arranging this electromagnet on the side of a recording disk opposite to its light incident side and lessening the restriction on the position of an optical system on the light incident side fo this recording disk. CONSTITUTION: An intensity change is applied to a laser beam by the optical modulator 4 according to the information to be recorded and this laser beam is converged by a converging lens 11. A recording track 23 is irradiated with this beam as a spot of about 1μm diameter. Curie point recording or coercive force recording is executed on the recording track 23 according to the intensity change of the laser beam. At this time, a magnetic field is generated by a coil 24 from the rear surface of the recording disk 12 and this magnetic field is impressed on the recording tack 23. The laser beam polarized to linearly polarized light is passed through Faraday glass 6 by a polarizing prism 5, by which an azimuth angle is rotated 45 deg. in the case reproduction of information is executed. The loss of the light quantity is minimized when the transmission axis of the next polarizing prism 7 is aligned to the azimuth angle of the polarized light after passing through the Faraday glass 6.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【発明の属する技術分野】本発明は垂直磁化膜に記録さ
れた情報をレーザ光を用いて再生する磁気光学記録再生
装量に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a magneto-optical recording / reproducing device for reproducing information recorded on a perpendicular magnetization film by using a laser beam.

【0002】近年、光メモリ装置は高密度、大容量、及
び高速アクセスの可能なメモリ装置として広く研究され
ているが、大別すると次の3種類が考えられる。
In recent years, an optical memory device has been widely studied as a memory device capable of high density, large capacity, and high speed access. When roughly classified, the following three types can be considered.

【0003】記憶素子に記録された情報の再生のみ可
能なもの。
A device that can only reproduce information recorded in a storage element.

【0004】再生及び情報の追加記録が可能なもの。Those capable of reproduction and additional recording of information.

【0005】再生・追加記録のみならず、不要な情報
を消去し、再記録することが可能なもの。
Not only reproduction / additional recording but also erasing unnecessary information and re-recording.

【0006】このうち、,の装置については既に実
用化の段階に至っているが、の装置については研究開
発段階にあり、実用化し得るものは皆無である。
Of these, the devices of and have already reached the stage of practical application, but the device of is at the stage of research and development, and there is nothing that can be put to practical use.

【0007】本発明はArレーザ、HeCdレーザ、H
eNeレーザ、半導体レーザ等のレーザ光を用いて熱磁
気的に情報の記録、消去を行い、又磁気光学効果を利用
して情報の再生を行うことにより、前記の装置の実用
化を図った磁気光学記録再生装置に関するものである。
The present invention is based on Ar laser, HeCd laser, H
Information is recorded and erased thermomagnetically by using a laser beam such as an eNe laser and a semiconductor laser, and information is reproduced by utilizing a magneto-optical effect. The present invention relates to an optical recording / reproducing device.

【0008】[0008]

【従来の技術】従来、磁気光学記録再生装置の実用的な
システムとして報告されているものは非常に少ない。
2. Description of the Related Art Very few conventional systems have been reported as practical systems for magneto-optical recording / reproducing devices.

【0009】実用に近いものとしては、電波新聞磁気メ
モリー特集電子テクノロジー(昭和55年9月18日発
行)がある。
As one close to practical use, there is the Denpa Newspaper Magnetic Memory Special Electronic Technology (published on September 18, 1980).

【0010】この記事では、鉄を主成分とした非晶質合
金の磁性薄膜をレーザの熱で、キュリー点まで温めるこ
とで、バイアス磁界の方向に磁化させることで書き込み
を行ない、一方直線偏光になったレーザビームを磁性薄
膜に入射し、それが反射する際に光の偏光面が磁化の向
きに依存して回転することを利用して、その回転状態を
検光子を介して測定することで情報を再生する装置が示
される。
In this article, writing is performed by heating a magnetic thin film of an amorphous alloy containing iron as a main component to the Curie point with the heat of a laser to magnetize the magnetic thin film in the direction of the bias magnetic field, while linearly polarized light is obtained. When the reflected laser beam is incident on the magnetic thin film and when it is reflected, the polarization plane of the light rotates depending on the direction of magnetization, and the rotation state is measured through an analyzer. A device for reproducing information is shown.

【0011】この装置の書き込みを行なう手段の構成を
概略説明すると、レーザー光源と、このレーザー光源か
ら発せられた光を光磁気ディスクに導くと共に光磁気デ
ィスクに光スポットを形成するレンズ等の光学系と、上
記光磁気ディスクと上記の光学系に含まれる光スポット
を光磁気ディスクに形成する集束レンズとの中間にあっ
て光磁気ディスクの磁性薄膜に外部からバイアス磁界を
印加するコイルからなる。
The structure of the writing means of this device will be briefly described. An optical system such as a laser light source and a lens for guiding light emitted from the laser light source to a magneto-optical disk and forming a light spot on the magneto-optical disk. And a coil for applying a bias magnetic field from the outside to the magnetic thin film of the magneto-optical disk in the middle of the magneto-optical disk and the focusing lens for forming a light spot included in the optical system on the magneto-optical disk.

【0012】[0012]

【発明が解決しようとする課題】しかし、この記事に示
される磁気光学記録再生装置の書き込みを行なう為の構
成では次の問題が生じた。
However, the structure for writing in the magneto-optical recording / reproducing apparatus shown in this article has the following problems.

【0013】即ち、集束レンズと光磁気ディスクの間に
コイルを配置した場合、コイルの厚みがある程度必要で
ある為に集束レンズと光磁気ディスクの間の距離を短く
できない。
That is, when a coil is arranged between the focusing lens and the magneto-optical disk, the distance between the focusing lens and the magneto-optical disk cannot be shortened because the coil needs a certain thickness.

【0014】逆に集束レンズと光磁気ディスクの間の距
離を適切な値にする為にはコイルの厚みを非常に薄くし
なければならず、その場合コイルの巻数を充分に取るこ
とができない。
On the contrary, in order to set the distance between the focusing lens and the magneto-optical disk to an appropriate value, the thickness of the coil must be made extremely thin, and in that case, the number of turns of the coil cannot be taken sufficiently.

【0015】又、コイルに電流を流して磁場を発生させ
る場合、永久磁石を用いる場合に比較して発生する磁場
の強度を充分に得ることが難しい。
Further, when an electric current is passed through the coil to generate a magnetic field, it is difficult to obtain a sufficient strength of the generated magnetic field as compared with the case where a permanent magnet is used.

【0016】その為に電流を大きくしたりコイルの巻数
を多くすることが必要となる。しかし電流を大きくする
ことは発熱が生ずる為に装置内の温度上昇につながり好
ましく無く、又、コイルの巻数を多くすることはそれに
よりインダクタンスが大きくなる為に磁場の応答変化が
遅くなり、光磁気ディスクに供給する磁場の高速切換が
困難になるという問題がある。
Therefore, it is necessary to increase the current and the number of turns of the coil. However, increasing the current is not preferable because it causes heat generation and raises the temperature in the device, and increasing the number of coil turns slows down the response change of the magnetic field due to the increase in the inductance, and There is a problem that high-speed switching of the magnetic field supplied to the disk becomes difficult.

【0017】[0017]

【課題を解決するための手段】本発明はこのような従来
問題点を解決するもので、レーザ光源と、透明な基板に
垂直磁化膜を形成してなる記録円板と、前記レーザ光源
から出射された光を記録情報に応じて光変調し、前記透
明な基板を介して垂直磁化膜にスポット照射させる光学
的手段とを有し、前記光変調されたスポット照射レーザ
光と電磁石から与えられた磁場により情報の記録を行な
う磁気光学記録再生装置において、前記情報記録時に前
記垂直磁化膜に磁場を供給するための、磁性体にコイル
を巻いて形成される電磁石を、前記記録円板の光入射側
とは反対側に配置してなることを特徴とするものであ
る。
SUMMARY OF THE INVENTION The present invention solves the above-mentioned conventional problems by providing a laser light source, a recording disk formed by forming a perpendicular magnetization film on a transparent substrate, and emitting from the laser light source. Optical means for optically modulating the generated light according to the recorded information and spot-irradiating the perpendicularly magnetized film through the transparent substrate, and the light-modulated spot-irradiating laser light and an electromagnet provided. In a magneto-optical recording / reproducing apparatus for recording information by a magnetic field, an electromagnet formed by winding a coil around a magnetic body for supplying a magnetic field to the perpendicularly magnetized film at the time of recording the information is incident on the recording disc. It is characterized in that it is arranged on the side opposite to the side.

【0018】[0018]

【発明の実施の形態】以下、本発明に係わる一実施例を
図面を用いて詳細に説明する。
BEST MODE FOR CARRYING OUT THE INVENTION An embodiment of the present invention will be described in detail below with reference to the drawings.

【0019】第1図は本発明に係わる磁気光学記録再生
装置の一実施例の簡略化した構成を示す図である。
FIG. 1 is a diagram showing a simplified construction of an embodiment of a magneto-optical recording / reproducing apparatus according to the present invention.

【0020】レーザ光源として気体レーザを用いた場合
を説明する。
A case where a gas laser is used as a laser light source will be described.

【0021】同図において、3はレーザ光源であり、こ
のレーザ光源3より出射され、記録すべき情報信号を光
に伝える光変調器4、直線偏光のみを通過させる偏光プ
リズム5、偏光面を回転させるファラディ効果素子6、
直線偏光のみを通過させる偏光プリズム7、ビームスプ
リッタ8、光路変更用ミラー9、λ/4板10、絞りレ
ンズ11、を通った光磁気光学記録円板12に入射され
る。この円板12からの帰り光は、上記絞りレンズ1
1、λ/4板10、ミラー9を通り、ビームスプリッタ
ー8により光路を変更して、λ/4板13、検光子14
を通過し受光素子15に入光する。又、記録、消去時に
記録素子に加える磁場は記録円板12の裏面より加える
ようにする。記録・消去・再生については後述する。
In FIG. 1, reference numeral 3 denotes a laser light source, which is an optical modulator 4 for transmitting an information signal to be recorded, which is emitted from the laser light source 3, a polarizing prism 5 for passing only linearly polarized light, and a polarization plane for rotation. Faraday effect element 6,
The light is incident on the magneto-optical recording disk 12 that has passed through a polarization prism 7, a beam splitter 8, an optical path changing mirror 9, a λ / 4 plate 10 and a diaphragm lens 11 that pass only linearly polarized light. The return light from the disc 12 is the diaphragm lens 1 described above.
1, the λ / 4 plate 10 and the mirror 9, and the optical path is changed by the beam splitter 8, and the λ / 4 plate 13 and the analyzer 14
And passes through to enter the light receiving element 15. The magnetic field applied to the recording element during recording and erasing is applied from the back surface of the recording disk 12. Recording / erasing / playback will be described later.

【0022】次に記録円板12は例えば第2図の断面図
に示すような構成とする。即ち厚さ0.5mmから2m
m程度の透明なガラス又は樹脂製の基板16にGdTb
Fe、TbFe等の希土類金属と遷移金属よりなるアモ
ルファスフェリ磁性体の垂直磁化膜17を形成し、更に
該アモルファス膜17の上にSiO2等の誘電体膜18
を形成し、該誘電体膜18上にAl、Au、Ag等の反
射膜19を形成し、ガラス、セラミック、金属、樹脂等
よりなる支持円板20を接着剤21で張り合わせた構成
とする。上記磁性体膜17にはあらかじめ結晶化により
形成されたガイドトラック22と磁気記録を行う記録ト
ラック23がある。この記録円板12はモーター28に
より所定の速度で回転される。
Next, the recording disc 12 is constructed as shown in the sectional view of FIG. 2, for example. Ie 0.5mm to 2m thick
GdTb on a transparent glass or resin substrate 16 of about m
A perpendicular magnetization film 17 of an amorphous ferrimagnetic material made of a transition metal and a rare earth metal such as Fe or TbFe is formed, and a dielectric film 18 such as SiO 2 is further formed on the amorphous film 17.
Is formed, a reflection film 19 of Al, Au, Ag, or the like is formed on the dielectric film 18, and a supporting disk 20 made of glass, ceramic, metal, resin, or the like is bonded with an adhesive 21. The magnetic film 17 has a guide track 22 previously formed by crystallization and a recording track 23 for magnetic recording. The recording disk 12 is rotated at a predetermined speed by a motor 28.

【0023】次に第1図に示す装置を用い情報の記録を
行う場合の説明をする。上記記録装置により情報の記録
を行うには記録すベき情報に応じて光変調器4により、
レーザ光に強度変化を与え、該レーザ光を絞りレンズ1
1により記録トラック23に約1μmφのスポットで絞
り照射する。そしてレーザ光の強度変化に応じて記録ト
ラック23上にキュリ点記録もしくは保磁力記録が行な
われる。この際に記録円板12の裏面からコイル24に
より磁場を発生させ、この磁場を記録トラック23に印
加する。
Next, the case of recording information using the apparatus shown in FIG. 1 will be described. In order to record information by the recording device, the optical modulator 4 according to the information to be recorded,
An intensity change is given to the laser light, and the laser light is stopped by the aperture lens 1
1, the recording track 23 is illuminated with a spot of about 1 μmφ. Curie point recording or coercive force recording is performed on the recording track 23 according to the change in the intensity of the laser beam. At this time, a magnetic field is generated from the back surface of the recording disk 12 by the coil 24, and this magnetic field is applied to the recording track 23.

【0024】上記コイル24はパーマロイ等の磁性体2
5に巻かれて電磁石とされている。
The coil 24 is made of a magnetic material 2 such as permalloy.
It is wound around 5 to make an electromagnet.

【0025】上記方法により情報は記録トラック23に
記録面に垂直上向き、又は垂直下向きの磁区として記録
される。
By the above method, the information is recorded on the recording track 23 as a magnetic domain which is vertically upward or vertically downward on the recording surface.

【0026】次に情報の再生を行う場合の説明をする。Next, a case of reproducing information will be described.

【0027】上記方法によ記録された情報の再生は、記
録されたトラックに偏光を入射させた時の反射光の偏光
状態及び反射光量の変化の、いわゆる磁気光学効果を利
用して行なわれる。
The reproduction of the information recorded by the above method is carried out by utilizing the so-called magneto-optical effect, which is the change in the polarization state and the amount of reflected light of reflected light when polarized light is incident on the recorded track.

【0028】第1図を参照して説明すれば、グラムトム
ソンプリズム等の偏光プリズム5により直線偏光になっ
たレーザ光はFR―5等のファラディガラス6を通過す
ることにより、方位角を45°回転させる。次の偏光プ
リズム7の透過軸をファラディガラス6の通過後の偏光
の方位角に合せると、光量の損失は極小におさえられ
る。偏光プリズム7を通過した光が記録トラック23上
に入射し、偏光状態及び光量の変化を受けて反射され、
ビームスプリッター8により受光器15ヘと導かれる。
その時検光子14の透過軸とλ/4板13の方位角を適
当に変化させ、記録状態に対応する信号雑音比(S/
N)が最も大きくなるよう調整する。λ/4板10も適
当に回転させS/Nを最大にするために用いる。
Referring to FIG. 1, the laser light linearly polarized by a polarizing prism 5 such as a Gram-Thomson prism passes through a Faraday glass 6 such as FR-5 to have an azimuth angle of 45 °. Rotate. When the transmission axis of the next polarizing prism 7 is adjusted to the azimuth angle of the polarized light after passing through the Faraday glass 6, the loss of the light quantity is suppressed to the minimum. The light that has passed through the polarization prism 7 is incident on the recording track 23, is reflected by the change in the polarization state and the light amount,
It is guided to the light receiver 15 by the beam splitter 8.
At that time, the transmission axis of the analyzer 14 and the azimuth angle of the λ / 4 plate 13 are appropriately changed, and the signal noise ratio (S / S) corresponding to the recording state is changed.
N) is adjusted to be the largest. The λ / 4 plate 10 is also used to appropriately rotate and maximize the S / N.

【0029】反射光は一般に楕円偏光になっているが、
偏光子7により楕円成分が除去され、ファラディガラス
6に入る。そしてファラディガラス6により方位角を4
5°進められた偏光は偏光プリズム5の通過軸と90°
の方位角をなすため、レーザ光源3の方向には帰らずC
の方向に反射される。
Although the reflected light is generally elliptically polarized light,
The elliptical component is removed by the polarizer 7 and enters the Faraday glass 6. And the azimuth is set to 4 by Faraday glass 6.
The polarized light advanced by 5 ° is 90 ° with the pass axis of the polarizing prism 5.
Since the azimuth angle of the laser light source 3 is formed,
Is reflected in the direction of.

【0030】尚、上記ファラディガラス6はリング状の
磁石26の中に入れられ磁石26の外側にコイル27を
巻いた構成にする。即ち磁石26によりファラディガラ
スの磁化をレーザ光線の方向に揃え、コイル27により
ファラディ回転角が45°になるよう補正する。従って
ファラディ効果素子の種類によっては磁石26のみある
いはコイル27のみでも良い場合がある。
The Faraday glass 6 is placed in a ring-shaped magnet 26, and a coil 27 is wound around the magnet 26. That is, the magnet 26 aligns the magnetization of the Faraday glass in the direction of the laser beam, and the coil 27 corrects the Faraday rotation angle to 45 °. Therefore, depending on the type of Faraday effect element, only the magnet 26 or the coil 27 may be sufficient.

【0031】以上の説明において、第1図は簡略図であ
り、フォーカストラック等のサーボに必要な光学系やレ
ーザ光を最適に絞るに必要なレンズ系は省略されてい
る。
In the above description, FIG. 1 is a simplified diagram, and the optical system necessary for servo of the focus track and the lens system necessary for optimally focusing the laser light are omitted.

【0032】又、上記記録再生の説明は気体レーザにつ
いて行なったが、半導体レーザを用いた場合の記録再生
は変調器4が不要である外はまったく同様に行なわれ
る。
Further, although the recording / reproducing has been described with respect to the gas laser, the recording / reproducing in the case of using the semiconductor laser is performed in exactly the same manner except that the modulator 4 is unnecessary.

【0033】又、上記説明では記録媒体として円板を用
いたが、膜面に垂直な磁化を有する記録媒体に磁区の形
で情報記録できるものであれば、本発明の主旨の範囲で
再生が可能であり、円板体の代わりにテープ状、ドラム
状、シート状等の記憶素子にでも適用できる。
Although a disk is used as the recording medium in the above description, reproduction is possible within the scope of the present invention as long as information can be recorded in the form of magnetic domains on a recording medium having a magnetization perpendicular to the film surface. This is also possible, and the present invention can also be applied to a tape-shaped, drum-shaped, sheet-shaped, or other storage element instead of a disc body.

【0034】[0034]

【発明の効果】以上の本発明によれば、レーザ光源と、
透明な基板に垂直磁化膜を形戒してなる記録円板と、前
記レーザ光源から出射された光を記録情報に応じて光変
調し、前記透明な基板を介して垂直磁化膜にスポット照
射させる光学的手段とを有し、前記光変調されたスポッ
ト照射レーザ光と電磁石から与えられた磁場により情報
の記録を行なう磁気光学記録再生装置において、前記情
報記録時に前記垂直磁化膜に磁場を供給するための、磁
性体にコイルを巻いて形成される電磁石を、前記記録円
板の光入射側とは反射側に配置したものであり、記録円
板の光入射側の光学系の位置的制約が少ない為、垂直磁
化膜に光変調してスポット照射させる為の集束レンズを
垂直磁化膜に充分近づけることができる。更に電磁石は
磁性体にコイルを巻いているので少ない電流で強い磁場
を発生することができ、熱の発生を抑制し、又リアクタ
ンスが少なくできるので電磁石から発生する磁場を高速
に制御することができる。
According to the present invention described above, a laser light source,
A recording disk formed by forming a perpendicular magnetic film on a transparent substrate, and light emitted from the laser light source is light-modulated according to recorded information, and the perpendicular magnetic film is spot-irradiated through the transparent substrate. In a magneto-optical recording / reproducing apparatus having optical means and recording information by the light-modulated spot irradiation laser light and a magnetic field given from an electromagnet, a magnetic field is supplied to the perpendicular magnetization film at the time of recording the information. Therefore, an electromagnet formed by winding a coil around a magnetic body is arranged on the light incident side of the recording disk and on the reflection side thereof, and there is a positional restriction of the optical system on the light incident side of the recording disk. Since the number is small, it is possible to bring the focusing lens for performing light modulation and spot irradiation on the perpendicular magnetic film sufficiently close to the perpendicular magnetic film. Furthermore, since the electromagnet has a coil wound around a magnetic body, it can generate a strong magnetic field with a small amount of current, suppress heat generation, and reduce reactance, so that the magnetic field generated from the electromagnet can be controlled at high speed. .

【図面の簡単な説明】[Brief description of drawings]

【図1】本発明に係わる磁気光学記録再生装置の一実施
例の基本的構成を示す図である。
FIG. 1 is a diagram showing a basic configuration of an embodiment of a magneto-optical recording / reproducing apparatus according to the present invention.

【図2】磁気光学記録円板の一例を示す一部拡大側面断
面図である。
FIG. 2 is a partially enlarged side sectional view showing an example of a magneto-optical recording disk.

【符号の説明】[Explanation of symbols]

3 レーザ光源 5、7 偏光プリズム 6 ファラディ効果素子 12 磁気光学記憶円板 3 Laser light source 5, 7 Polarizing prism 6 Faraday effect element 12 Magneto-optical storage disk

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 レーザ光源と、 透明な基板に垂直磁化膜を形成してなる記録円板と、 前記レーザ光源から出射された光を記録情報に応じて光
変調し、前記透明な基板を介して垂直磁化膜にスポット
照射させる光学的手段とを有し、 前記光変調されたスポット照射レーザ光と電磁石から与
えられた磁場により情報の記録を行なう磁気光学記録再
生装置において、 前記情報記録時に前記垂直磁化膜に磁場を供給するため
の、磁性体にコイルを巻いて形成される電磁石を、前記
記録円板の光入射側とは反対側に配置してなることを特
徴とする磁気光学記録再生装置。
1. A laser light source, a recording disk comprising a transparent substrate on which a perpendicularly magnetized film is formed, and light emitted from the laser light source is optically modulated in accordance with recording information, and is transmitted through the transparent substrate. An optical means for irradiating a spot on a perpendicularly magnetized film, and performing information recording by the magnetic field applied from the light-modulated spot irradiating laser light and an electromagnet. Magneto-optical recording / reproducing, characterized in that an electromagnet formed by winding a coil around a magnetic body for supplying a magnetic field to the perpendicularly magnetized film is arranged on the side opposite to the light incident side of the recording disk. apparatus.
JP7305287A 1995-11-24 1995-11-24 Magneto-optical recording / reproducing device Expired - Lifetime JP2744776B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP7305287A JP2744776B2 (en) 1995-11-24 1995-11-24 Magneto-optical recording / reproducing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7305287A JP2744776B2 (en) 1995-11-24 1995-11-24 Magneto-optical recording / reproducing device

Related Parent Applications (1)

Application Number Title Priority Date Filing Date
JP14063090A Division JPH03198242A (en) 1990-05-30 1990-05-30 Magneto-optical recording and reproducing device

Publications (2)

Publication Number Publication Date
JPH08227542A true JPH08227542A (en) 1996-09-03
JP2744776B2 JP2744776B2 (en) 1998-04-28

Family

ID=17943289

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7305287A Expired - Lifetime JP2744776B2 (en) 1995-11-24 1995-11-24 Magneto-optical recording / reproducing device

Country Status (1)

Country Link
JP (1) JP2744776B2 (en)

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5495250A (en) * 1978-01-11 1979-07-27 Kokusai Denshin Denwa Co Ltd Heat magnetic recording system

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5495250A (en) * 1978-01-11 1979-07-27 Kokusai Denshin Denwa Co Ltd Heat magnetic recording system

Also Published As

Publication number Publication date
JP2744776B2 (en) 1998-04-28

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