JPS59215008A - Optical magnetic disc device - Google Patents

Optical magnetic disc device

Info

Publication number
JPS59215008A
JPS59215008A JP8749683A JP8749683A JPS59215008A JP S59215008 A JPS59215008 A JP S59215008A JP 8749683 A JP8749683 A JP 8749683A JP 8749683 A JP8749683 A JP 8749683A JP S59215008 A JPS59215008 A JP S59215008A
Authority
JP
Japan
Prior art keywords
recording
magnetic field
optical
signal
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
JP8749683A
Other languages
Japanese (ja)
Other versions
JPH053642B2 (en
Inventor
Yasuyuki Tamura
泰之 田村
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.)
Canon Inc
Original Assignee
Canon Inc
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 Canon Inc filed Critical Canon Inc
Priority to JP8749683A priority Critical patent/JPS59215008A/en
Publication of JPS59215008A publication Critical patent/JPS59215008A/en
Publication of JPH053642B2 publication Critical patent/JPH053642B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B11/00Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor
    • G11B11/10Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field
    • G11B11/105Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing

Landscapes

  • Recording Or Reproducing By Magnetic Means (AREA)

Abstract

PURPOSE:To obtain an optical magnetic disc device which makes the best of the optical modulating system and the magnetic field modulating system in one device by recording many high speed data by the optical modulation system and recording a few data such as management information or the like by the magnetic field modulation system. CONSTITUTION:The image of an optical beam irradiated from a semiconductor laser 1 is formed on an optomagnetic recording medium 6 through a collimator lens 3, a mirror 4 and an objective lens 5. In recording information at high speed, the optical modulation system is adopted, a recording signal is given through a signal line L1, a semiconductor laser 1 is driven in response to the recording signal by means of a laser driver 2 so as to modulate the optical beam. Then the temperature of a part on which the optical beam is irradiated rises, the magnetization is inverted and the signal is recorded. In recording data at comparatively low speed, the mode is changed over into the magnetic field modulating system, optical beams of a prescribed level are generated continuously from the laser 1 by means of the laser driver 2 and a current changed in forward/reverse direction in response to the recording signal is given to a coil 10 via a coil driver 11 from a signal line L2, then an alternating magnetic field is generated and the information is recorded.

Description

【発明の詳細な説明】 技術分野 本発明は磁気光学効果を利用して情報信号の記録再生を
行う光磁気ディスク装置に関する。
DETAILED DESCRIPTION OF THE INVENTION Technical Field The present invention relates to a magneto-optical disk device that records and reproduces information signals using magneto-optic effects.

従来技術 光磁気ディスク装置では、一般にGd’TbFeあるい
ハcd−CO等の磁性体薄膜に磁界および光ビームを作
用させて磁化の向きを変化させることにより情報信号を
記録し、再生にあたっては、直線偏光のレーザ光を磁性
体薄膜に照射し1反射または透過したときに磁気カー効
果、あるいはファラデー効果により直線偏光光の光の振
動面が磁化の向きに従って回転することを利用して記録
信号を読み出している。なお、媒体の表面で反射した光
が回転するのを磁気カー効果、透過した光が回転するの
をファラデー効果という。
In conventional magneto-optical disk drives, information signals are generally recorded by applying a magnetic field and a light beam to a magnetic thin film such as Gd'TbFe or Hcd-CO to change the direction of magnetization. When a linearly polarized laser beam is irradiated onto a magnetic thin film and reflected or transmitted, the recording signal is recorded by utilizing the magnetic Kerr effect or Faraday effect, which causes the vibration plane of the linearly polarized light to rotate according to the direction of magnetization. Reading out. The rotation of light reflected from the surface of a medium is called the magnetic Kerr effect, and the rotation of transmitted light is called the Faraday effect.

特に、光磁気ディスク装置は極めて大容量であり、かつ
高速度で曹き込みおよび再生が可能であり、かつVTR
や磁気ディスクと同様に消去会再書き込みができる等の
多くの利点な有するので。
In particular, magneto-optical disk devices have an extremely large capacity, can be loaded and played back at high speed, and are compatible with VTRs.
It has many advantages, such as the ability to erase and rewrite data just like magnetic disks.

画像情報の記録装置等として期待されている。It is expected to be used as a recording device for image information.

このように、光磁気ディスク装置における記録信号(デ
ータ)の書き込み方式とじてヲ了、従来からコつの方式
が知られている。まず、第1の記録方式としてヲ1.記
録信号に応じて変調されたレーザビームを磁性体薄膜か
らなるディスク面に照射して、情報を記録する方式があ
る。この場合には。
As described above, there are conventionally known methods for writing recording signals (data) in magneto-optical disk devices. First, the first recording method is 1. There is a method of recording information by irradiating a disk surface made of a magnetic thin film with a laser beam modulated according to a recording signal. In this case.

一般にレーザビームの照射と同時に変調されていない磁
界をディスク面に加えることによりディスクの磁化感度
を高め、比較的弱いレーザビームで記録することを可能
圧している。しかし、このような磁界を印加しなくても
、レーザビームが強ければ記録することができるの12
勿論である。以下。
Generally, by applying an unmodulated magnetic field to the disk surface simultaneously with laser beam irradiation, the magnetization sensitivity of the disk is increased, making it possible to record with a relatively weak laser beam. However, even without applying such a magnetic field, recording is possible if the laser beam is strong12
Of course. below.

この第7の記録方式を光変調方式と称する。This seventh recording method is called a light modulation method.

第コの記録方式として汀、変調されていない光ビームを
磁性体薄膜からなるディスク面に照射し。
The first recording method is to irradiate an unmodulated light beam onto a disk surface made of a thin magnetic film.

これと同時に記録信号に応じて変調された磁界を加える
方式がある。その際に印加する磁界を、それ自体の磁界
強度では、記録できない程度の弱い磁界とすることによ
り、光ビームの照射されている部分にのみ情報を正確に
記録することができるようにしている。なお、その磁界
を1.記録部近傍に配設したコイルに、記録信号に応じ
た電流を流すことにより発生する。以下この第コの記録
方式を磁界変調方式と称する。
At the same time, there is a method of applying a magnetic field modulated according to the recording signal. By making the magnetic field applied at this time so weak that it cannot record with its own magnetic field strength, information can be accurately recorded only in the area irradiated with the light beam. In addition, the magnetic field is 1. It is generated by passing a current corresponding to a recording signal through a coil disposed near the recording section. Hereinafter, this No. 1 recording method will be referred to as a magnetic field modulation method.

従来の光磁気ディスク装置においては、上述の一つの記
録方式の内のいずれか一方を用いていた。
Conventional magneto-optical disk devices have used one of the above-mentioned recording methods.

上述の一つの記録方式を比較すると、極めて高速かつ高
密度の記録を行うには、光変調方式の方が適している。
Comparing the above-mentioned recording methods, the optical modulation method is more suitable for extremely high-speed and high-density recording.

磁界変調方式では、コイルに高速度の記録信号を与えな
ければならないが、コイルは所定のインダクタンスを有
するため、高速度の信号をあたえることは困難であるか
らである。しかしながら。
In the magnetic field modulation method, it is necessary to apply a high-speed recording signal to the coil, but since the coil has a predetermined inductance, it is difficult to apply a high-speed signal. however.

光変調方式では1丁でに記録されている部分の記録デー
タの変更を行う時に次のような欠点が有る。
The optical modulation method has the following drawbacks when changing the recorded data of a portion recorded in one device.

すなわち、光変調方式では1丁でに記録された部分に直
接新たなデータを書き込むことを1できず。
In other words, with the optical modulation method, it is not possible to directly write new data to the previously recorded area.

記録された部分を一度消去し、しかる後に新たなデータ
を書き込む必要が有る。そのため、データの変更に商っ
ては消去および再書き込みの一行程を必要とする。
It is necessary to erase the recorded portion once and then write new data. Therefore, changing data requires one process of erasing and rewriting.

他方、磁界変調方式で%1丁でに記録された部分であっ
ても、消去行程な経ずに直接に新たなデータを書き込む
ことができる利点がある。
On the other hand, there is an advantage that new data can be directly written to a portion recorded using the magnetic field modulation method without going through an erasing process.

このように、光磁気ディスク装置を大容量の画像データ
ファイル等として用いる場合には、高速度で高密度の記
録および再生をしなければならないため、従来の磁界変
調方式は不適切であり、光変調方式を用いるのが適して
いる。しかし、そのような記録および再生を行なう場合
には、ディスク上のどのエリア(領域)に、どのような
画像の情報が記録されているか、あるい)Xディスク上
のどのエリアが丁でに使用されているか等のいわゆる管
理情報をも、一つの光磁気ディスク装置により同一のデ
ィスク上に記録しておく必要が有る。
In this way, when using a magneto-optical disk device for large-capacity image data files, etc., it is necessary to perform high-speed, high-density recording and reproducing, so conventional magnetic field modulation methods are inappropriate, and optical It is suitable to use a modulation method. However, when performing such recording and playback, it is important to know what kind of image information is recorded in which area on the disk, or which area on the X disk is currently being used. It is also necessary to record so-called management information, such as information on whether or not the data is being stored, on the same disk using a single magneto-optical disk device.

ところが、そのような管理情報はしばしば更新する必要
が生ずるので、随時必要に応じて書き替えを行う必要が
有るが、上述のように直接書き込みができない光変調方
式汀、この管理情報の記録に4不適切であるという問題
がある。
However, since such management information often needs to be updated, it is necessary to rewrite it from time to time as necessary. There is a problem with inappropriateness.

目   的 そこで1本発明の目的舎工、上述した欠点を除去し、7
つの装置で高速大量のデータを光変調方式で記録し、管
理情報等の少量データを磁界変調方式で記録することに
より1両方式の利点を生かした光磁気ディスク装置を提
供することにある。
Purpose: 1. The purpose of the present invention is to eliminate the above-mentioned drawbacks, and to
An object of the present invention is to provide a magneto-optical disk device that takes advantage of the advantages of both methods by recording a large amount of data at high speed using an optical modulation method and recording a small amount of data such as management information using a magnetic field modulation method in one device.

かかる目的を達成するために本発明は、レーザビームを
記録信号に応じて変調する光ビーム変調手段と、光ビー
ムの照射位置に磁界を発生する磁界発生手段と、その磁
界を記録信号に応じて変調する磁界変調手段とを有する
光磁気ディスク装置を提供するものである。
In order to achieve such an object, the present invention comprises: a light beam modulator that modulates a laser beam according to a recording signal; a magnetic field generator that generates a magnetic field at a position irradiated with the light beam; The present invention provides a magneto-optical disk device having a magnetic field modulating means for modulating the magnetic field.

実施例 以下1図面を参照して本発明の詳細な説明する。Example The present invention will be described in detail below with reference to one drawing.

第7図は本発明光磁気ディスク装置の構成の−例を示し
、ここで、/ケレーザビームを発射−fる半導体レーザ
1.2は半導体レーザlを駆動するレーザドライバであ
り、レーザドライバーを1信号線L/を通じて供給され
る記録信号に応じてレーザビームを変調する。3を丁半
導体レーザーから出たレーザビームを平行光線束にする
コリメータレンズ、4It”zレーザビームの光路を変
える反射ミラー。
FIG. 7 shows an example of the configuration of a magneto-optical disk device of the present invention, in which a semiconductor laser 1.2 that emits a laser beam is a laser driver that drives a semiconductor laser l, and the laser driver is driven by one signal. The laser beam is modulated in response to a recording signal provided through line L/. 3 is a collimator lens that converts the laser beam emitted from the semiconductor laser into a bundle of parallel rays, and 4 is a reflective mirror that changes the optical path of the laser beam.

s trsレーザビームをスポット状に集光する対物レ
ンズである。
This is an objective lens that focuses the strs laser beam into a spot.

6 K’S円盤状の光磁気記録媒体(光磁気ディスク)
であり、その記録面はGd=TbFeあるいI工Cd 
C。
6 K'S disk-shaped magneto-optical recording medium (magneto-optical disk)
, and its recording surface is Gd=TbFe or I/Cd
C.

等の磁性体薄膜で形成され、対物レンズSで集光された
レーザビームスポットが照射される。りはその光磁気記
録媒体6を所定の回転速度で駆動する駆動モータである
。ざは反射ミラーグとコリメータレンズ3の間に介在し
て、光磁気記録媒体6上で反射されたレーザビームの反
射光を分割するハーフミラ−19はハーフミラ−tを通
った上述の反射光を受光してそのフォーカス状態を検出
するフォーカス検知光学系であり、このフォーカス検知
光学系9は1例えば集光レンズ、波長板(偏光板)およ
びCCD等の受光素子(光電変換素子)とを有する。
A laser beam spot focused by an objective lens S is irradiated with the laser beam spot. This is a drive motor that drives the magneto-optical recording medium 6 at a predetermined rotational speed. The half mirror 19, which is interposed between the reflecting mirror and the collimator lens 3 and splits the reflected light of the laser beam reflected on the magneto-optical recording medium 6, receives the above-mentioned reflected light that has passed through the half mirror t. This focus detection optical system 9 includes, for example, a condenser lens, a wavelength plate (polarizing plate), and a light receiving element (photoelectric conversion element) such as a CCD.

さらに、lθは光磁気記録媒体芯の光ビームの照射位置
に磁界を与える磁界発生用コイル、iiはこの磁界発生
用コイル10を駆動するコイルドライパテアリ、コイル
ドライバ//に1信号11L:1を通じて供給される記
録信号に応じてコイル10の磁界を変調する。
Furthermore, lθ is a magnetic field generation coil that applies a magnetic field to the irradiation position of the light beam on the magneto-optical recording medium core, ii is a coil dryer that drives this magnetic field generation coil 10, and 1 signal 11L:1 is sent to the coil driver //. The magnetic field of the coil 10 is modulated according to the recording signal supplied through the coil 10.

次に、動作を説明すると、半導体レーザlから発した光
ビームI工、コリメーターレンズ3.ミラー+、および
対物レンズ5を通って、光磁気記録媒体6上に直径約−
μm程度のスポット状に結像される。光磁気記録媒体6
面での反射光の一部は。
Next, to explain the operation, the light beam emitted from the semiconductor laser I, the collimator lens 3. Through the mirror + and the objective lens 5, a diameter of approximately −
The image is formed into a spot on the order of μm. Magneto-optical recording medium 6
Some of the light reflected by the surface.

ハーフミラ−gによりフォーカス検知光学系tに導かれ
、その光学系9の受光により対物レンズSと光磁気記録
媒体6間の距離の誤差信号を得、この誤差信号に応じて
対物レンズ5を上下方向に移 ・ 動して、光磁気配録
媒体6上に正確にスポットを結像する。
The light is guided to the focus detection optical system t by the half mirror g, and an error signal of the distance between the objective lens S and the magneto-optical recording medium 6 is obtained by receiving the light from the optical system 9, and the objective lens 5 is moved in the vertical direction according to this error signal.・ Move to accurately form a spot on the magneto-optical recording medium 6.

対物レンズSの近傍&Cは図示のように磁界発生用コイ
ルIOが設けてあり、一方、光磁気記録媒体Aげモータ
フによって例えばlざθ(7r、p、mで回転されてい
る。さらに、半導体レーザー/、光学系3.’l、!、
g、9およびコイル/θ等は不図示のハウジング内に収
納され、記録再生ヘッドとして光磁気記録媒体芯の半径
方向に対して一体的に移動可能となっており、それによ
り光磁気記録媒体芯の任意の位置に記録データを書き込
むことができる。
Near the objective lens S &C, a magnetic field generating coil IO is provided as shown in the figure, and on the other hand, the magneto-optical recording medium A is rotated by, for example, l.theta.(7r, p, m).Furthermore, a semiconductor Laser/, optical system 3.'l,!,
g, 9, coil /θ, etc. are housed in a housing (not shown), and are movable integrally in the radial direction of the magneto-optical recording medium core as a recording/reproducing head. Recording data can be written to any location in the memory.

以上の構成により、高速度で情報を記録する時には、光
変調方式を採用して信号線L/を通じて記録信号を与え
、レーザドライバλによりその記録信号に応じて、半導
体レーザ/を駆動し、光ビームを変調する。この時、コ
イル1OKk’!コイルドライバl/から一定の直流電
流を流して、光磁気記録媒体6が予め磁化されている方
向と逆方向の磁界を発生させても良く、また光ビームが
強ければコイルドライバ//に通電しなくても良い。
With the above configuration, when recording information at a high speed, an optical modulation method is adopted to provide a recording signal through the signal line L/, and the laser driver λ drives the semiconductor laser/ in accordance with the recording signal, thereby producing light. Modulate the beam. At this time, coil 1 OKk'! A constant DC current may be passed from the coil driver l/ to generate a magnetic field in the opposite direction to the direction in which the magneto-optical recording medium 6 is magnetized in advance, and if the light beam is strong, the coil driver l/ is energized. You don't have to.

これにより、光ビームの当った部分の温度が局所的に上
昇して磁化が反転し゛、倍信号記録される。
As a result, the temperature of the portion hit by the light beam locally increases, the magnetization is reversed, and a double signal is recorded.

このようにして記録した光磁気記録媒体6上の記録信号
を消去する時には、コイルドライバコに上述と逆極性の
直流電流を通電し、予め磁化されている方向と同じ方向
、つまり記録ピットと逆方向の磁界をコイルIOにより
発生し、それと同時に一定の光ビームを照射することに
より、記録信号を消去する。このように、光変調方式に
より記録を行い、−fでに記録された部分(記録ビット
)を書きかえるには、その前に予め記録信号の消去を行
う必要が有る・ 一方、比較的低速のデータ(例えば、前述の管理情報等
)を記録する時には、不図示のスイッチング手段により
磁界変調方式に切り換え、レーザードライバーによりレ
ーザlから一定レベルの光ビームを連続して発生させ、
これと同時に信号線Lコを通じて記録信号をコイルドラ
イバ/lに与え、コイルドライバl/から記録信号に芯
じて正逆方向に変化する電流をコイルlθに通電し、記
録信号に応じた交番磁界を発生する。これにより。
When erasing the recorded signal on the magneto-optical recording medium 6 recorded in this way, a DC current of the opposite polarity to that described above is applied to the coil driver coil in the same direction as the previously magnetized direction, that is, opposite to the recording pit. The recorded signal is erased by generating a directional magnetic field by the coil IO and simultaneously irradiating a constant light beam. In this way, in order to perform recording using the optical modulation method and rewrite the recorded part (recorded bits) with -f, it is necessary to erase the recorded signal in advance. When recording data (for example, the above-mentioned management information, etc.), the switching means (not shown) switches to the magnetic field modulation method, and the laser driver continuously generates a light beam of a certain level from the laser l.
At the same time, a recording signal is given to the coil driver /l through the signal line L, and a current that changes in the forward and reverse directions with respect to the recording signal is passed from the coil driver l to the coil lθ, thereby producing an alternating magnetic field according to the recording signal. occurs. Due to this.

光ビームの当った部分は記録信号に応じて、磁化の方向
が反転し、情報が記録される。この磁界変調方式で記録
する時には、その記録部分にすでに記録されたデータが
有るか否かにかかわらず記録することができ、記録情報
の消去の必要がない。
The direction of magnetization of the portion hit by the light beam is reversed in accordance with the recording signal, and information is recorded. When recording using this magnetic field modulation method, it is possible to record regardless of whether or not there is already recorded data in the recording area, and there is no need to erase the recorded information.

このように本例では一つの装置で1画像情報等の主情報
を高速度で記録することと、低速でもよい管理情報等の
補助的情報を消去せずに書き換えることとの両方ができ
るので、実用上非常に便利となる。実際に使用するとき
には、記録すべきデータを高速で記録し、それに応じて
管理情報を低速で書き換えるなどが好適である。
In this way, in this example, one device can both record main information such as one image information at high speed, and rewrite auxiliary information such as management information, which may be performed at low speed, without erasing it. This is very convenient in practice. In actual use, it is preferable to record the data to be recorded at high speed and rewrite the management information at low speed accordingly.

なお、記録された情報を読み出すとき[4工、前述した
従来のような単一の情報読み出し手段によって行うこと
ができ、上述の2つの方式のそれぞ ゛れに対して独立
に読み出し手段を設ける必要はない。ただし、変調信号
の復調にあたってヲ工、それぞれの方式の記録時の変調
方式にあわせて行うことが必要であるのは勿論である。
It should be noted that when reading out the recorded information, it can be done by a single information reading means like the conventional one described above, and a reading means is provided independently for each of the two methods mentioned above. There's no need. However, it goes without saying that the demodulation of the modulated signal must be performed in accordance with the modulation method used for each recording method.

さらに1本例における一つの記録方式によって記録する
部分の領域を、記録媒体6上に記録方式別にそれぞれ区
分して予め定めて置くことは、有効である。この場合に
、記録媒体感の内側中心部を磁界変調方式に割当て、配
録媒体乙の外側近傍を光変調方式f割当るとよい。
Furthermore, it is effective to divide and predetermine areas of the portion to be recorded by one recording method on the recording medium 6 according to each recording method in this example. In this case, it is preferable to allocate the inner central part of the recording medium to the magnetic field modulation method, and the outer vicinity of the recording medium B to the optical modulation method f.

すなわち、光変調方式での記録速度の限界は。In other words, what are the limits to the recording speed of optical modulation methods?

記録媒体6上の記録ピットの大きさによって制限を受け
る。つまり、記録信号に応じて形成される記録ピットハ
、確実に独立して形成される範囲内で記録する必要があ
るからである。そこで、記録媒体6が一定回転数で回転
している時rtXその外側はど線速度が高く、高速記録
が可能となる。一方、磁界変調方式でヲ工、コイルio
のインダクタンスによって、記録速度が制限される。つ
まり。
It is limited by the size of recording pits on the recording medium 6. In other words, it is necessary to ensure that the recording pits formed according to the recording signal are recorded within the range where they are formed independently. Therefore, when the recording medium 6 is rotating at a constant rotational speed, the linear velocity outside the rtX is high, making high-speed recording possible. On the other hand, with the magnetic field modulation method, the coil
The recording speed is limited by the inductance. In other words.

コイルlθのインダクタンスのために、高速度でコイル
IOに流れる電流を変化させることが困難であり、それ
によって記録速度が制限をうけるからである。したがっ
て、記録媒体感の内側中心部であっても外側周辺部であ
っても、記録速度の上限はほぼ変らないこととなる。
This is because it is difficult to change the current flowing through the coil IO at a high speed due to the inductance of the coil lθ, which limits the recording speed. Therefore, the upper limit of the recording speed remains almost the same whether it is at the inner center of the recording medium or at the outer periphery.

よって、磁界変調方式によって記録する部分を記録媒体
感の内側に設定することにより、一つの記録媒体感に対
し、より多(のデータを記録することができる。なお、
記録する部分に応じて、モータ7の回転数を変化させる
場合であっても、上述力ように記録領域を区分して設定
することにより、モータ7の回転数の可変幅をより小さ
くすることができる利点もある。
Therefore, by setting the portion to be recorded using the magnetic field modulation method inside the recording medium, more data can be recorded on one recording medium.
Even when changing the rotation speed of the motor 7 depending on the area to be recorded, by setting the recording area in sections as described above, the variable range of the rotation speed of the motor 7 can be made smaller. There are some advantages to doing so.

効果 以上説明したように1本発明によれば、一つの装置で、
情報の高速度の記録と、データの書きがえを簡易に行な
う記録との両方を実現することができる効果が得られる
Effects As explained above, according to the present invention, with one device,
This provides the effect of realizing both high-speed recording of information and recording that allows data to be easily rewritten.

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

第1図は本発明光磁気ディスク装置の構成の一例を示す
概略構成図である。 l・・・半導体レーザ。 コ・・・レーザドライバ。 3・・・コリメータレンズ。 ダ・・・反射ミラー。 j・・・対物レンズ。 6・・・光磁気記録媒体。 7・・・モータ。 g・・・ハーフミラ−。 デ・パフオーカス検知光学系。 10…コイル、 l/・・・コイルドライバ。 L/、L、2・・・信号線。 特許出願人   キャノン株式会社
FIG. 1 is a schematic configuration diagram showing an example of the configuration of a magneto-optical disk device of the present invention. l...Semiconductor laser. Co...Laser driver. 3... Collimator lens. Da... reflective mirror. j...Objective lens. 6... Magneto-optical recording medium. 7...Motor. g...Half mirror. De Paf Orcus detection optical system. 10...Coil, l/...Coil driver. L/, L, 2...Signal line. Patent applicant Canon Co., Ltd.

Claims (1)

【特許請求の範囲】 /)光磁気記録媒体と、光ビームを発生する光源と、該
光源から発した前記光ビームを前記光磁気記録媒体上に
照射する光学系と、前記光ビームを第1の記録信号に応
じて変調する光ビーム変調手段と、前記光ビームの照射
位置に磁界を発生する磁界発生手段と、前記磁界を第コ
の記録信号に応じて変調する磁界変調手段と、前記記録
信号を前記光ビーム変調手段または前記磁界変調手段の
いずれか一方に切換えて供給する信号供給切換手段とを
具備したことを特徴とする光磁気ディスク装置。 コ)特許請求の範囲第1項記載の装置におい【。 前記光磁気記録媒体に前記記録信号を記録する時に該光
磁気記録媒体の回転中心部において前配光ビームを一定
に保ち、前記記録信号に応じて前記磁界を変調し、該光
磁気記録媒体の回転周辺srおいて前記磁界を一定に保
ち、前記光ビームを前記記録信号に応じて変調するよう
に制御する制御手段とを有することを特徴とする光磁気
ディスク装置。
[Scope of Claims] /) A magneto-optical recording medium, a light source that generates a light beam, an optical system that irradiates the light beam emitted from the light source onto the magneto-optical recording medium, and a first a light beam modulating means for modulating the magnetic field according to the recording signal; a magnetic field generating means for generating a magnetic field at the irradiation position of the light beam; a magnetic field modulating means for modulating the magnetic field according to the recording signal; A magneto-optical disk device comprising: a signal supply switching means for switching and supplying a signal to either the light beam modulation means or the magnetic field modulation means. f) In the apparatus according to claim 1 [. When recording the recording signal on the magneto-optical recording medium, the front light distribution beam is kept constant at the center of rotation of the magneto-optical recording medium, the magnetic field is modulated according to the recording signal, and the magnetic field is modulated in accordance with the recording signal. A magneto-optical disk device comprising: control means for controlling the magnetic field to be constant in the rotational periphery sr, and for controlling the light beam to be modulated in accordance with the recording signal.
JP8749683A 1983-05-20 1983-05-20 Optical magnetic disc device Granted JPS59215008A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8749683A JPS59215008A (en) 1983-05-20 1983-05-20 Optical magnetic disc device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8749683A JPS59215008A (en) 1983-05-20 1983-05-20 Optical magnetic disc device

Related Child Applications (2)

Application Number Title Priority Date Filing Date
JP31227193A Division JPH076445A (en) 1993-12-13 1993-12-13 Magneto-optical recording and reproducing device
JP5312270A Division JP2540012B2 (en) 1993-12-13 1993-12-13 Magneto-optical recording / reproducing device

Publications (2)

Publication Number Publication Date
JPS59215008A true JPS59215008A (en) 1984-12-04
JPH053642B2 JPH053642B2 (en) 1993-01-18

Family

ID=13916573

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8749683A Granted JPS59215008A (en) 1983-05-20 1983-05-20 Optical magnetic disc device

Country Status (1)

Country Link
JP (1) JPS59215008A (en)

Cited By (13)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61187141A (en) * 1985-02-14 1986-08-20 Nec Corp Photomagnetic recording system
JPS61190741A (en) * 1985-02-19 1986-08-25 Nec Corp Photomagnetic recording medium
JPS61190743A (en) * 1985-02-19 1986-08-25 Nec Corp Photomagnetic recording system
JPS61190742A (en) * 1985-02-19 1986-08-25 Nec Corp Photomagnetic recording medium
JPS61190740A (en) * 1985-02-19 1986-08-25 Nec Corp Photomagnetic recording system
DE3802693A1 (en) * 1987-01-30 1988-08-11 Hitachi Ltd Magneto=optical recording system
WO1989008914A1 (en) * 1988-03-10 1989-09-21 Storage Technology Corporation Apparatus for writing data on a magneto-optic recording medium
JPH02249158A (en) * 1989-03-23 1990-10-04 Matsushita Electric Ind Co Ltd Recording and reproducing device
US5043960A (en) * 1987-09-25 1991-08-27 Hitachi, Ltd. Overwritable magneto-optic recording and reproducing apparatus
US5105408A (en) * 1988-05-12 1992-04-14 Digital Equipment Corporation Optical head with flying lens
EP0576286A2 (en) * 1992-06-26 1993-12-29 Canon Kabushiki Kaisha Magnetic head driving device and magnetooptical recording apparatus
US5434831A (en) * 1990-01-23 1995-07-18 Canon Kabushiki Kaisha Magneto-optical recording apparatus capable of both magnetic modulation and light modulation recording
US5689478A (en) * 1992-10-09 1997-11-18 Canon Kabushiki Kaisha Magnetic head for magneto-optical recording and magneto-optical recording apparatus in which a magnetic core mounted to a slider has particular dimensions and properties

Citations (4)

* 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
JPS5766537A (en) * 1980-10-09 1982-04-22 Sharp Corp Magnetooptic recording and reproducing device
JPS57117106A (en) * 1981-01-09 1982-07-21 Olympus Optical Co Ltd Optical magnetic recording and reproducing method
JPS57189302A (en) * 1981-05-18 1982-11-20 Fujitsu Ltd Optical magnetic recording system

Patent Citations (4)

* 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
JPS5766537A (en) * 1980-10-09 1982-04-22 Sharp Corp Magnetooptic recording and reproducing device
JPS57117106A (en) * 1981-01-09 1982-07-21 Olympus Optical Co Ltd Optical magnetic recording and reproducing method
JPS57189302A (en) * 1981-05-18 1982-11-20 Fujitsu Ltd Optical magnetic recording system

Cited By (14)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61187141A (en) * 1985-02-14 1986-08-20 Nec Corp Photomagnetic recording system
JPS61190741A (en) * 1985-02-19 1986-08-25 Nec Corp Photomagnetic recording medium
JPS61190743A (en) * 1985-02-19 1986-08-25 Nec Corp Photomagnetic recording system
JPS61190742A (en) * 1985-02-19 1986-08-25 Nec Corp Photomagnetic recording medium
JPS61190740A (en) * 1985-02-19 1986-08-25 Nec Corp Photomagnetic recording system
DE3802693A1 (en) * 1987-01-30 1988-08-11 Hitachi Ltd Magneto=optical recording system
US5043960A (en) * 1987-09-25 1991-08-27 Hitachi, Ltd. Overwritable magneto-optic recording and reproducing apparatus
WO1989008914A1 (en) * 1988-03-10 1989-09-21 Storage Technology Corporation Apparatus for writing data on a magneto-optic recording medium
US5105408A (en) * 1988-05-12 1992-04-14 Digital Equipment Corporation Optical head with flying lens
JPH02249158A (en) * 1989-03-23 1990-10-04 Matsushita Electric Ind Co Ltd Recording and reproducing device
US5434831A (en) * 1990-01-23 1995-07-18 Canon Kabushiki Kaisha Magneto-optical recording apparatus capable of both magnetic modulation and light modulation recording
EP0576286A2 (en) * 1992-06-26 1993-12-29 Canon Kabushiki Kaisha Magnetic head driving device and magnetooptical recording apparatus
EP0576286A3 (en) * 1992-06-26 1994-08-10 Canon Kk Magnetic head driving device and magnetooptical recording apparatus
US5689478A (en) * 1992-10-09 1997-11-18 Canon Kabushiki Kaisha Magnetic head for magneto-optical recording and magneto-optical recording apparatus in which a magnetic core mounted to a slider has particular dimensions and properties

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