JPH0512780B2 - - Google Patents

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Publication number
JPH0512780B2
JPH0512780B2 JP2140630A JP14063090A JPH0512780B2 JP H0512780 B2 JPH0512780 B2 JP H0512780B2 JP 2140630 A JP2140630 A JP 2140630A JP 14063090 A JP14063090 A JP 14063090A JP H0512780 B2 JPH0512780 B2 JP H0512780B2
Authority
JP
Japan
Prior art keywords
recording
magneto
optical
disk
magnetic field
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.)
Expired - Lifetime
Application number
JP2140630A
Other languages
Japanese (ja)
Other versions
JPH03198242A (en
Inventor
Kenji Oota
Toshihisa Deguchi
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
Application filed by Sharp Corp filed Critical Sharp Corp
Priority to JP14063090A priority Critical patent/JPH03198242A/en
Publication of JPH03198242A publication Critical patent/JPH03198242A/en
Publication of JPH0512780B2 publication Critical patent/JPH0512780B2/ja
Granted legal-status Critical Current

Links

Description

【発明の詳細な説明】 <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置に関す
る。
DETAILED DESCRIPTION OF THE INVENTION <Technical Field> The present invention relates to a magneto-optical recording and reproducing device that reproduces information recorded on a perpendicularly magnetized film using a laser beam.

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, optical memory devices have been widely studied as high-density, large-capacity, and high-speed access memory devices, and the following three types can be considered.

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 memory element.

再生及び情報の追加記録が可能なもの。 Something that can be played back and additionally recorded.

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。
In addition to playback and additional recording, it is also possible to erase unnecessary information and re-record.

このうち、、の装置については既に実用化
の段階に至つているが、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 in . have already reached the stage of practical use, but the devices in .

本発明はArレーザ、HeCdレーザ、HeNe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
置の実用化を図つた磁気光学記録再生装置に関す
るものである。
The present invention records and erases information thermomagnetically using a laser beam such as an Ar laser, HeCd laser, HeNe laser, or semiconductor laser, and reproduces the information using the magneto-optic effect. The present invention relates to a magneto-optical recording/reproducing device which aims to put the device into practical use.

<従来技術> 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。
<Prior Art> Until now, very few practical systems of magneto-optical recording and reproducing devices have been reported.

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。
An example of something close to practical use is the Dempa Shimbun Magnetic Memory Special Feature on Electronic Technology (published on September 18, 1980).

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、キユリー点まで温める
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、一方直線偏光になつたレーザ
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 made of an amorphous alloy mainly composed of iron to the Curie point using laser heat, and magnetizing it in the direction of a bias magnetic field. A beam is incident on a magnetic thin film, and when it is reflected, the plane of polarization of the light rotates depending on the direction of magnetization. Information is reproduced by measuring the state of rotation using an analyzer. The device that does this is shown.

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イスクに導くと共に
光磁気デイスクに光スポツトを形成するレンズ等
の光学系と、上記光磁気デイスクと上記の光学系
に含まれる光スポツトを光磁気デイスクに形成す
る集束レンズとの中間にあつて光磁気デイスクの
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 explained: a laser light source, an optical system such as a lens that guides the light emitted from the laser light source to the magneto-optical disk and forms a light spot on the magneto-optical disk, and the above-mentioned optical system. It consists of a coil that is located between the magneto-optical disk and a focusing lens that forms an optical spot included in the optical system on the magneto-optical disk, and applies a bias magnetic field from the outside to the magnetic thin film of the magneto-optical disk.

<発明が解決しようとする問題点> 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。
<Problems to be Solved by the Invention> However, the following problems arose in the configuration for writing in the magneto-optical recording/reproducing device shown in this article.

即ち、集束レンズと光磁気デイスクの間にコイ
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イスクの間の距
離を短くできない。
That is, when a coil is placed 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 must be thick to some extent.

逆に集束レンズと光磁気デイスクの間の距離を
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
に有ることができない。
Conversely, 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 very thin, and in this case, the number of turns of the coil cannot be sufficient.

又、コイルに電流を流して磁場を発生させる場
合、氷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。
Furthermore, when a magnetic field is generated by passing a current through a coil, it is difficult to obtain a sufficient strength of the generated magnetic field compared to when using a Hikyu magnet.

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、光磁気デイスク
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 or increase the number of turns of the coil. However, increasing the current is undesirable because it generates heat, which increases the temperature inside the device, and increasing the number of turns in the coil increases the inductance, which slows down the response change of the magnetic field and magneto-optically. There is a problem in that it becomes difficult to quickly switch the magnetic field supplied to the disk.

<問題点を解決する為の手段> 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前記透明な
基板を介して垂直磁化膜にスポツト照射させる光
学的手段と、 前記記録円板の光入射側とは反射側にあつて、
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
とを備え、 レーザ光線から出射されたレーザ光と電磁石か
ら与えられ磁場により情報の記録を行なうことを
特徴とするものである。
<Means for Solving the Problems> The present invention solves these conventional problems, and includes: a laser light source; a recording disk formed by forming a perpendicularly magnetized film on a transparent substrate; an optical means for spot-irradiating the emitted light onto the perpendicularly magnetized film through the transparent substrate; and a light incident side of the recording disk is a reflective side,
An electromagnet formed by winding a coil around a magnetic material is provided to supply a magnetic field to the perpendicularly magnetized film during information recording, and information is recorded using the laser beam emitted from the laser beam and the magnetic field provided by the electromagnet. It is characterized by this.

<実施例> 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。
<Example> Hereinafter, an example according to the present invention will be described in detail using the drawings.

第1図は本発明に係わる磁気光学記憶再生装置
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 configuration of an embodiment of a magneto-optical storage/reproduction device according to the present invention.

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 will be described in which a gas laser is used as the laser light source.

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アラデ
イ効果素子6、直線偏光のみを通過させる偏光プ
リズム7、ビームスプリツタ8、光路変更用ミラ
ー9、λ/4板10、絞りレンズ11、を通つた
光が磁気光学記憶円板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11、
λ/4板10、ミラー9を通り、ビームスプリツ
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 the figure, 3 is a laser light source, an optical modulator 4 that is emitted from the laser light source 3 and transmits an information signal to be recorded into the light, a polarizing prism 5 that passes only linearly polarized light, and a Faraday effect that rotates the plane of polarization. Light that has passed through the element 6, the polarizing prism 7 that allows only linearly polarized light to pass through, the beam splitter 8, the optical path changing mirror 9, the λ/4 plate 10, and the aperture lens 11 is incident on the magneto-optic storage disk 12. The returning light from this disk 12 is transmitted through the aperture lens 11,
The light passes through a λ/4 plate 10 and a mirror 9, has its optical path changed by a beam splitter 8, passes through a λ/4 plate 13 and an analyzer 14, and enters a light receiving element 15. or,
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/
Reproduction will be described later.

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2mm程
度の透明なガラス又は樹脂製の基板16に
GdTbFe、TbFe等の希土類金属と遷移金属より
なるアモルフアスフエリ磁性体の垂直磁化膜17
を形成し、更に該アモルフアス膜17の上に
SiO2等の誘電体膜18を形成し、該誘電体膜1
8上にAl、Au、Ag等の反射膜19を形成し、ガ
ラス、セラミツク、金属、樹脂等よりなる支持円
板20を接着剤21で張り合せた構成とする。上
記磁性体膜17にはあらかじめ結晶化により形成
されたガイドトラツク22と磁気記録を行う記録
トラツク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 disk 12 has a structure as shown in the sectional view of FIG. 2, for example. That is, on a transparent glass or resin substrate 16 with a thickness of about 0.5 mm to 2 mm.
Perpendicular magnetization film 17 of amorphous ferrimagnetic material made of rare earth metals such as GdTbFe and TbFe and transition metals
is formed on the amorphous film 17.
A dielectric film 18 such as SiO 2 is formed, and the dielectric film 1
A reflective film 19 made of Al, Au, Ag, etc. is formed on 8, and a support disk 20 made of glass, ceramic, metal, resin, etc. is pasted together with an adhesive 21. The magnetic film 17 has a guide track 22 formed in advance by crystallization and a recording track 23 for performing magnetic recording. This recording disk 12 is rotated by a motor 28 at a predetermined speed.

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。
Next, a case where information is recorded using the apparatus shown in FIG. 1 will be explained.

上記記憶装置により情報の記録を行うには記録
すべ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11
により記録トラツク23に約1μmφのスポツト
で絞り照射する。そしてレーザ光の強度変化に応
じて記録トラツク23上にキユリ点記録もしくは
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
の磁場を記録トラツク23に印加する。
To record information using the storage device, the optical modulator 4 changes the intensity of the laser beam according to the information to be recorded, and the laser beam is focused through the aperture lens 11.
The recording track 23 is irradiated with a spot of approximately 1 μmφ. Curling point recording or coercive force recording is then performed on the recording track 23 in response to changes in the intensity of the laser beam. At this time, the recording disk 12
A magnetic field is generated by a coil 24 from the back side of the recording track 23, and this magnetic field is applied to the recording track 23.

上記コイル24はパーマロイ等の磁性体25に
巻かれて電磁石とされている。
The coil 24 is wound around a magnetic material 25 such as permalloy to form an electromagnet.

上記方法により情報は記録トラツク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, information is recorded on the recording track 23 as magnetic domains pointing vertically upward or vertically downward to the recording surface.

次に情報の再生を行う場合の説明をする。 Next, the case of reproducing information will be explained.

上記方法により記録された情報の再生は、記録
されたトラツ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。
Reproduction of information recorded by the above method is carried out by utilizing the so-called magneto-optic effect, which is a change in the polarization state of reflected light and the amount of reflected light when polarized light is incident on a recorded track.

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
つたレーザ光はFR−5等のフアラデイガラス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の透過軸をフアラデイガラス
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
した光が記録トラツク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
ツター8により受光器15へと導かれる。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。
To explain with reference to FIG. 1, the laser beam, which has been linearly polarized by a polarizing prism 5 such as a Gram-Thompson prism, is transmitted through a Faraday glass 6 such as FR-5.
By passing through, the azimuth is rotated by 45°.
By aligning the transmission axis of the next polarizing prism 7 with the azimuth of the polarized light after passing through the Faraday glass 6, the loss of light amount can be minimized. The light that has passed through the polarizing prism 7 is incident on the recording track 23, is reflected as the polarization state and light amount changes, and is guided to the light receiver 15 by the beam splitter 8. At this time, the transmission axis of the analyzer 14 and the azimuth angle of the λ/4 plate 13 are appropriately changed to adjust the signal-to-noise ratio (S/N) corresponding to the recording state to be the largest. λ/
The four plates 10 are also rotated appropriately and used to maximize the S/N ratio.

反射光は一般に楕円偏光になつているが、偏光
子7により楕円成分が除去され、フアラデイガラ
ス6に入る。そしてフアラデイガラス6により方
位角を45゜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。
The reflected light is generally elliptically polarized light, but the elliptical component is removed by the polarizer 7 and enters the Faraday glass 6. The polarized light whose azimuth angle has been advanced by 45 degrees by the Faraday glass 6 makes an azimuth angle of 90 degrees with the passage axis of the polarizing prism 5, so it is not returned to the direction of the laser light source 3 but is reflected in the direction C.

尚、上記フアラデイガラス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によりフアラ
デイガラスの磁化をレーザ光線の方向に揃え、コ
イル27によりフアラデイ回転角が45゜になるよ
う補正する。従つてフアラデイ効果素子の種類に
よつては磁石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 inside a ring-shaped magnet 26, and a coil 27 is placed outside the magnet 26.
Create a rolled configuration. 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 degrees. Therefore, depending on the type of Faraday effect element, only the magnet 26 or only the coil 27 may be sufficient.

以上の説明において、第1図は簡略図であり、
フオーカストラツ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 explanation, FIG. 1 is a simplified diagram,
Optical systems necessary for servo such as focus tracks and lens systems necessary to optimally focus the laser beam are omitted.

又、上記記録再生の説明は気体レーザについて
行なつたが、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つたく同様に行
なわれる。
Furthermore, although the above description of recording and reproducing has been made with respect to a gas laser, recording and reproducing when a semiconductor laser is used is performed in exactly the same way except that the modulator 4 is not required.

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。
Furthermore, although a disk was used as the recording medium in the above explanation, 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 that has magnetization perpendicular to the film surface. , instead of a disk, the present invention can be applied to a tape-shaped, drum-shaped, sheet-shaped memory element, etc.

<効果> 以上の本発明によれば、レーザ光源から出射さ
れた光を透明な基板を介して記録円板の垂直磁化
膜にスポツト照射させ、記録円板の光入射側とは
反対側に位置する磁性体にコイルを巻いて形成さ
れる電磁石を備えるようにしたので、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
磁化膜にスポツ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るから熱の発生
を抑制でき、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の向きを切換る際に高速
に磁場を切換ることができるものである。
<Effects> According to the present invention described above, the light emitted from the laser light source is spot irradiated onto the perpendicularly magnetized film of the recording disk through the transparent substrate, and the perpendicularly magnetized film of the recording disk is spot-irradiated on the side opposite to the light incident side of the recording disk. Since it is equipped with an electromagnet formed by winding a coil around a magnetic material, there are fewer positional constraints on the optical system on the light incident side of the recording disk, so the focusing lens for spot irradiating the perpendicularly magnetized film can be placed perpendicularly. It can be brought sufficiently close to the magnetized film. Furthermore, since the electromagnet has a coil wound around a magnetic material, it is possible to generate a strong magnetic field with a small amount of current, which can suppress the generation of heat.Also, because the reactance can be reduced, the direction of the magnetic field generated by the electromagnet can be switched at high speed. It is possible to switch the magnetic field to

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

第1図は本発明に係わる磁気光学記録再生装置
の一実施例の基本的構成を示す図、第2図は磁気
光学記憶円板の一例を示す一部拡大側面断面図で
ある。 図中、3:レーザ光源、5,7:偏光プリズ
ム、6:フアラデイ効果素子、12:磁気光学記
憶円板。
FIG. 1 is a diagram showing the basic configuration of an embodiment of a magneto-optical recording/reproducing apparatus according to the present invention, and FIG. 2 is a partially enlarged side sectional view showing an example of a magneto-optic storage disk. In the figure, 3: laser light source, 5, 7: polarizing prism, 6: Faraday effect element, 12: magneto-optic storage disk.

Claims (1)

【特許請求の範囲】 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前記透明な
基板を介して垂直磁化膜にスポツト照射させる光
学的手段と、 前記記録円板の光入射側とは反射側にあつて、
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
とを備え、 レーザ光源から出射されたレーザ光と電磁石か
ら与えられ磁場により情報の記録を行なうことを
特徴とする磁気光学記録再生装置。
[Claims] 1. A laser light source, a recording disk formed by forming a perpendicularly magnetized film on a transparent substrate, and spot irradiation of light emitted from the laser light source onto the perpendicularly magnetized film via the transparent substrate. an optical means for causing the recording disk, and the light incident side of the recording disk is on the reflective side,
An electromagnet formed by winding a coil around a magnetic material is provided for supplying a magnetic field to the perpendicularly magnetized film during information recording, and information is recorded using a laser beam emitted from a laser light source and a magnetic field provided by the electromagnet. A magneto-optical recording and reproducing device characterized by:
JP14063090A 1990-05-30 1990-05-30 Magneto-optical recording and reproducing device Granted JPH03198242A (en)

Priority Applications (1)

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

Applications Claiming Priority (1)

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

Related Parent Applications (1)

Application Number Title Priority Date Filing Date
JP55141553A Division JPS5766537A (en) 1980-10-09 1980-10-09 Magnetooptic recording and reproducing device

Related Child Applications (1)

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

Publications (2)

Publication Number Publication Date
JPH03198242A JPH03198242A (en) 1991-08-29
JPH0512780B2 true JPH0512780B2 (en) 1993-02-18

Family

ID=15273164

Family Applications (1)

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

Country Status (1)

Country Link
JP (1) JPH03198242A (en)

Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5191711A (en) * 1975-02-10 1976-08-11
JPS5421709A (en) * 1977-07-19 1979-02-19 Fuji Photo Film Co Ltd Thermomagnetic recording system
JPS55122244A (en) * 1979-03-07 1980-09-19 Nippon Hoso Kyokai <Nhk> Photomagnetic recording and reproducing method
JPS5625470A (en) * 1979-08-09 1981-03-11 Mitsubishi Electric Corp Photo beam thermomagnetic recording apparatus
JPS56117345A (en) * 1980-02-22 1981-09-14 Nippon Hoso Kyokai <Nhk> Optical recording medium

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6426281A (en) * 1987-01-07 1989-01-27 Seiko Epson Corp Image reading device

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5191711A (en) * 1975-02-10 1976-08-11
JPS5421709A (en) * 1977-07-19 1979-02-19 Fuji Photo Film Co Ltd Thermomagnetic recording system
JPS55122244A (en) * 1979-03-07 1980-09-19 Nippon Hoso Kyokai <Nhk> Photomagnetic recording and reproducing method
JPS5625470A (en) * 1979-08-09 1981-03-11 Mitsubishi Electric Corp Photo beam thermomagnetic recording apparatus
JPS56117345A (en) * 1980-02-22 1981-09-14 Nippon Hoso Kyokai <Nhk> Optical recording medium

Also Published As

Publication number Publication date
JPH03198242A (en) 1991-08-29

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