JPH05347042A - Method for magneto-optical recording - Google Patents
Method for magneto-optical recordingInfo
- Publication number
- JPH05347042A JPH05347042A JP18037392A JP18037392A JPH05347042A JP H05347042 A JPH05347042 A JP H05347042A JP 18037392 A JP18037392 A JP 18037392A JP 18037392 A JP18037392 A JP 18037392A JP H05347042 A JPH05347042 A JP H05347042A
- Authority
- JP
- Japan
- Prior art keywords
- recording
- magneto
- optical recording
- magnetic field
- medium
- 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
Abstract
Description
【0001】[0001]
【産業上の利用分野】本発明は磁界変調方式による光磁
気記録方法に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a magneto-optical recording method using a magnetic field modulation method.
【0002】[0002]
【従来の技術】光磁気記録方法の記録方式のひとつに磁
界変調方式がある。この方式は、光磁気記録媒体に変調
した磁界を与えるとともに記録パワーを一定に保ったレ
ーザ光を照射して記録を行う方式である。この磁界変調
方式による光磁気記録方法では、オーバーライトが可能
であることから、従来必要であった消去プロセスは必要
なくなり、記録、ベリファイの2つのプロセスとなるの
で、転送レートが早くなるといったメリットをもつ。2. Description of the Related Art A magnetic field modulation method is one of recording methods of a magneto-optical recording method. This system is a system in which recording is performed by applying a modulated magnetic field to a magneto-optical recording medium and irradiating a laser beam whose recording power is kept constant. In the magneto-optical recording method using the magnetic field modulation method, since overwriting is possible, the erasing process that has been conventionally required is not necessary, and two processes of recording and verifying are performed, which has the advantage of increasing the transfer rate. Hold.
【0003】[0003]
【発明が解決しようとする課題】しかしながら、近年の
情報処理の高速化の要望にこたえるためには、さらに転
送レートの高速化が必要で、そのためには、ディスク回
転数を早くしたり、線密度を上げるなどの方法がある
が、いずれも限界がある。さらに、古いデータの上にオ
ーバーライトする時、古いデータを記録した時よりも低
い記録パワーで記録すると、消し残りが生じ、エラーが
頻繁に発生する恐れがある。However, in order to meet the recent demand for high-speed information processing, it is necessary to further increase the transfer rate. For that purpose, the disk rotation speed is increased and the linear density is increased. There are ways to raise it, but there are limits. Furthermore, when overwriting on old data, if data is recorded with a lower recording power than that when old data is recorded, unerased data may remain and errors may occur frequently.
【0004】本発明はこのような従来技術の問題点を解
決するためになされたもので、転送レートのより一層の
向上を図ることができ、かつ確実なオーバーライトが可
能な光磁気記録方法を提供することを目的とする。The present invention has been made to solve the above-mentioned problems of the prior art, and provides a magneto-optical recording method capable of further improving the transfer rate and capable of reliable overwriting. The purpose is to provide.
【0005】[0005]
【課題を解決するための手段】上記目的を達成するた
め、本発明によれば、光磁気記録媒体に変調した磁界を
与えるとともに記録パワーを一定に保ったレーザ光を照
射して記録を行う磁界変調方式による光磁気記録方法に
おいて、記録動作中に、光磁気記録媒体からの反射回折
光を2分割フォトダイオードを介して取り出した信号か
ら得た和信号をモニターし、その結果に基づいて、記録
を終了するか、あるいは異なる領域に再度記録を行うか
を決定することを特徴とする光磁気記録方法が提供され
る。また、本発明によれば、上記において、和信号に対
して一定のしきい値を設けておき、モニターした和信号
が該しきい値を越えた区間を欠陥区間とし、その区間と
対応するパルスの幅をクロックで計測することにより光
磁気記録媒体の欠陥数及び欠陥長を求め、得られた結果
に基づいて、記録を終了するか、あるいは異なる領域に
再度記録を行うかを決定することを特徴とする光磁気記
録方法が提供される。また、本発明によれば、光磁気記
録媒体に変調した磁界を与えるとともに記録パワーを一
定に保ったレーザ光を照射して記録を行う磁界変調方式
による光磁気記録方法において、記録動作中に、光磁気
記録媒体からの反射回折光を2分割フォトダイオードを
介して取り出した信号から得た差信号をモニターし、そ
の結果に基づいて、記録を終了するか、あるいは記録条
件を変更して再度記録を行うかを決定することを特徴と
する光磁気記録方法が提供される。さらに、本発明によ
れば、上記において、差信号に対して一定のしきい値を
設けておき、モニターした差信号が該しきい値を越えた
時に記録レーザパワーを上げることにより再度記録を行
うことを特徴とする光磁気記録方法が提供される。In order to achieve the above object, according to the present invention, a magnetic field for recording by applying a modulated magnetic field to a magneto-optical recording medium and irradiating a laser beam whose recording power is kept constant. In a magneto-optical recording method using a modulation method, a sum signal obtained from a signal obtained by extracting reflected diffracted light from a magneto-optical recording medium through a two-division photodiode is monitored during a recording operation, and recording is performed based on the result. The present invention provides a magneto-optical recording method characterized by deciding whether to end recording or to perform recording again in a different area. Further, according to the present invention, in the above, a constant threshold value is provided for the sum signal, and a section in which the monitored sum signal exceeds the threshold value is defined as a defect section, and a pulse corresponding to the section. The number of defects and the length of the defect in the magneto-optical recording medium are obtained by measuring the width of the clock with a clock, and based on the obtained results, it is possible to decide whether to end the recording or to perform the recording again in a different area. A featured magneto-optical recording method is provided. Further, according to the present invention, in a magneto-optical recording method by a magnetic field modulation method for performing recording by applying a modulated magnetic field to a magneto-optical recording medium and irradiating with laser light whose recording power is kept constant, during a recording operation, The difference signal obtained from the signal obtained by extracting the reflected diffracted light from the magneto-optical recording medium through the two-division photodiode is monitored, and based on the result, the recording is ended or the recording condition is changed and the recording is performed again. There is provided a magneto-optical recording method characterized by deciding whether to perform. Further, according to the present invention, in the above, a constant threshold value is provided for the difference signal, and when the monitored difference signal exceeds the threshold value, the recording laser power is increased to perform the recording again. A magneto-optical recording method is provided.
【0006】[0006]
【作用】和信号は媒体に欠陥があると信号強度が変動
し、差信号は消し残りがあるおそれを反映して大きくな
る。従って、記録動作中に和信号あるいは差信号(両方
でもよい)をモニターすることにより、欠陥の状況、消
し残りの状況を知ることができ、その状況に応じて別の
セクターに再記録する、記録レーザパワーを上げて再記
録する等の適切な処理を行うことができる。従って、転
送レートの向上と確実なオーバーライトが実現でき、前
記課題が解決される。When the medium has a defect, the signal intensity fluctuates, and the difference signal becomes large reflecting the possibility that there is an unerased portion. Therefore, by monitoring the sum signal or the difference signal (both may be used) during the recording operation, it is possible to know the defect status and the unerased status, and re-record in another sector according to the status. Appropriate processing such as increasing the laser power and re-recording can be performed. Therefore, the transfer rate can be improved and reliable overwrite can be realized, and the above problems can be solved.
【0007】[0007]
【実施例】以下本発明を実施例に基づき詳細に説明す
る。図1は光磁気記録再生装置の光学系を模式的に示す
図で、1は半導体レーザ(LD)、2はコリメータレン
ズ、3はビームシェーパー、4は第2のビームスプリッ
タ、5は第1のビームスプリッタ、6はミラープリズ
ム、7は対物レンズ、8は1/2波長板、9は偏波ビー
ムスプリッタ、10はコリメータレンズ、11は第1の
フォトダイオード、12はコリメータレンズ、13は第
2のフォトダイオードである。本発明の方法は、光磁気
記録媒体に変調した磁界を与えるとともに記録パワーを
一定に保ったレーザ光を照射して記録を行う磁界変調方
式により記録を行い、しかも光磁気記録媒体からの反射
回折光を2分割フォトダイオード(図1の11、13)
を介して取り出した信号から得た和信号又は差信号をモ
ニターして記録の制御を行う。ここで、和信号とは第1
のフォトダイオード11の出力と第2のフォトダイオー
ド13の出力の和をとった信号であり、差信号とは第1
のフォトダイオード11の出力と第2のフォトダイオー
ド13の出力の差をとった信号である。通常、和信号は
媒体にプレピットとして存在するIDを読むのに使用さ
れ、差信号は光磁気記録した記録マークを再生するため
に使用される。EXAMPLES The present invention will be described in detail below based on examples. FIG. 1 is a diagram schematically showing an optical system of a magneto-optical recording / reproducing apparatus. 1 is a semiconductor laser (LD), 2 is a collimator lens, 3 is a beam shaper, 4 is a second beam splitter, and 5 is a first beam splitter. Beam splitter, 6 is a mirror prism, 7 is an objective lens, 8 is a half-wave plate, 9 is a polarization beam splitter, 10 is a collimator lens, 11 is a first photodiode, 12 is a collimator lens, and 13 is a second lens. It is a photodiode of. According to the method of the present invention, recording is performed by a magnetic field modulation method in which a modulated magnetic field is applied to a magneto-optical recording medium and a laser beam whose recording power is kept constant is applied to perform recording, and reflection diffraction from the magneto-optical recording medium is performed. Photodiode that splits light into two (11 and 13 in Fig. 1)
The recording is controlled by monitoring the sum signal or the difference signal obtained from the signal taken out via. Here, the sum signal is the first
Is a signal obtained by summing the output of the photodiode 11 and the output of the second photodiode 13, and the difference signal is the first
Is a signal obtained by taking the difference between the output of the photodiode 11 and the output of the second photodiode 13. Normally, the sum signal is used to read the ID existing as prepits on the medium, and the difference signal is used to reproduce the recording mark recorded magneto-optically.
【0008】まず、和信号のモニターによる制御につい
て説明する。記録パワーを一定に保ったレーザ光を光磁
気記録媒体に照射すると、媒体の反射率に応じた信号強
度(図2のV)の和信号が得られる。図2に示すように
この和信号は媒体に欠陥があると信号強度が変化する。
そこで、この和信号の信号強度に対して、あるしきい値
を設けておき、それを越えた区間を欠陥区間とし、その
区間と対応するパルスの幅をクロックにより計測すれ
ば、媒体の欠陥数、欠陥長が得られる。従って、記録動
作中に和信号をモニターして媒体の欠陥数、欠陥長を計
測し、それが訂正不能な欠陥長であったり、あるセクタ
ー内に欠陥数が一定以上ある場合には、交代セクターに
再記録し、そのようなことがなければベリファイなしに
記録を終える。このような制御を可能とするために、例
えば、ドライブ側に、和信号を入力しそのレベルがしき
い値を越えた区間をクロックにより計測する第1の回路
と、該第1の回路により計測された欠陥数と欠陥長を記
憶する第2の回路と、許容される欠陥数及び欠陥長を予
め記憶している第3の回路と、第2の回路と第3の回路
の内容を比較して、ベリファイなしに記録を終えるか、
交代セクターへの再記録を行うかを決定する第4の回路
を設ければよい。このような機能を有する各回路の設計
自体は周知の技術を用いて行うことができる。First, the control by the monitor of the sum signal will be described. When a magneto-optical recording medium is irradiated with laser light whose recording power is kept constant, a sum signal of signal intensities (V in FIG. 2) according to the reflectance of the medium is obtained. As shown in FIG. 2, this sum signal changes in signal strength when the medium has a defect.
Therefore, if a threshold value is set for the signal strength of this sum signal, a section that exceeds the threshold value is set as a defect section, and the pulse width corresponding to that section is measured by a clock, the number of defects in the medium is determined. , The defect length can be obtained. Therefore, the sum signal is monitored during the recording operation to measure the number of defects and the defect length of the medium, and if the defect length is uncorrectable or the number of defects in a certain sector exceeds a certain level, the replacement sector Re-record to, and if there is no such case, the recording ends without verification. In order to enable such control, for example, a first circuit that inputs a sum signal to the drive side and measures a section in which the level exceeds a threshold value by a clock, and a measurement by the first circuit The contents of the second circuit and the third circuit are compared with the second circuit that stores the number of defects and the defect length that are stored, the third circuit that stores the number of defects and the defect length that are allowed in advance. To finish recording without verifying,
It suffices to provide a fourth circuit for determining whether to perform re-recording on the alternate sector. The design itself of each circuit having such a function can be performed using a known technique.
【0009】次に、差信号のモニターによる制御につい
て説明する。記録動作中に得られる差信号は、図3に示
すように、レーザスポット内の領域において、媒体の熱
伝導によりスポットの前方では媒体温度が高く、スポッ
トの後方では温度が低くなっている。そしてキュリー温
度(Tc)以上の領域は磁化を消失しているため、差信
号にあらわれるのはスポットの後方域の古いデータが記
録してある領域となる。記録パワーが低いとスポットの
後方域から得られる信号強度は大きいが、記録レーザパ
ワーが高くなるとキュリー温度に近づくため信号強度は
低下する。そこで、この差信号に対して、あるしきい値
を設けておき、差信号の信号強度がそのしきい値を越え
た時には、例えば記録パワーを上げて再度記録を行うよ
うにすると、古いデータの信号強度を小さく或いは完全
に消去でき、確実にオーバーライトすることができるよ
うになる。このような制御を可能にするには、例えば、
ドライブ側に、差信号を入力しそのレベルがしきい値を
越えたか否かを判定する回路と、該回路により差信号の
レベルがしきい値を越えた時に適切な記録パワーへの変
更及び再記録を指示する回路を設ければよい。このよう
な機能を有する各回路の設計自体は周知の技術を用いて
行うことができる。Next, the control by monitoring the difference signal will be described. As shown in FIG. 3, the difference signal obtained during the recording operation has a high medium temperature in front of the spot and a low temperature in the rear of the spot due to heat conduction of the medium in the region inside the laser spot. Since the magnetization disappears in the area above the Curie temperature (Tc), the difference signal appears in the area where old data is recorded in the area behind the spot. When the recording power is low, the signal intensity obtained from the rear area of the spot is high, but when the recording laser power is high, the signal intensity decreases because the Curie temperature approaches. Therefore, a threshold value is set for this difference signal, and when the signal strength of the difference signal exceeds the threshold value, for example, the recording power is increased and recording is performed again. The signal strength can be reduced or completely erased, and overwrite can be surely performed. To enable such control, for example,
A circuit for determining whether or not the level of the difference signal exceeds a threshold value by inputting the difference signal to the drive side and a circuit for changing and rewriting to an appropriate recording power when the level of the difference signal exceeds the threshold value. A circuit for instructing recording may be provided. The design itself of each circuit having such a function can be performed using a known technique.
【0010】[0010]
【発明の効果】以上詳細に説明したように、本発明によ
れば、和信号あるいは差信号をモニターすることによ
り、記録動作中に欠陥検査、消し残り検査を行うことが
でき、これによりベリファイが必要なくなり、転送レー
トのより一層の向上が図れるとともに、確実なオーバー
ライトが可能となる。As described above in detail, according to the present invention, by monitoring the sum signal or the difference signal, it is possible to perform a defect inspection and an unerased inspection during the recording operation, and thereby verify. It is not necessary, the transfer rate can be further improved, and reliable overwrite is possible.
【図1】光磁気記録再生装置の光学系を模式的に示す図
である。FIG. 1 is a diagram schematically showing an optical system of a magneto-optical recording / reproducing device.
【図2】和信号のモニターによる制御の説明図である。FIG. 2 is an explanatory diagram of control by monitoring a sum signal.
【図3】差信号のモニターによる制御の説明図である。FIG. 3 is an explanatory diagram of control by monitoring a difference signal.
1 半導体レーザ 2 コリメータ
レンズ 3 ビームシェーパー 4 第2のビー
ムスプリッタ 5 第1のビームスプリッタ 6 ミラープリ
ズム 7 対物レンズ 8 1/2波長
板 9 偏波スプリッタ 10 コリメータ
レンズ 11 第1のフォトダイオード 12 コリメー
タレンズ 13 第2のフォトダイオード1 Semiconductor Laser 2 Collimator Lens 3 Beam Shaper 4 Second Beam Splitter 5 First Beam Splitter 6 Mirror Prism 7 Objective Lens 8 1/2 Wave Plate 9 Polarization Splitter 10 Collimator Lens 11 First Photodiode 12 Collimator Lens 13 Second photodiode
Claims (4)
とともに記録パワーを一定に保ったレーザ光を照射して
記録を行う磁界変調方式による光磁気記録方法におい
て、記録動作中に、光磁気記録媒体からの反射回折光を
2分割フォトダイオードを介して取り出した信号から得
た和信号をモニターし、その結果に基づいて、記録を終
了するか、あるいは異なる領域に再度記録を行うかを決
定することを特徴とする光磁気記録方法。1. A magneto-optical recording method according to a magnetic field modulation method, wherein a modulated magnetic field is applied to a magneto-optical recording medium and recording is performed by irradiating a laser beam whose recording power is kept constant. The sum signal obtained from the signal obtained by extracting the reflected diffracted light from the medium through the two-division photodiode is monitored, and based on the result, it is determined whether the recording is ended or the recording is performed again in a different area. A magneto-optical recording method characterized by the above.
おき、モニターした和信号が該しきい値を越えた区間を
欠陥区間とし、その区間と対応するパルスの幅をクロッ
クで計測することにより光磁気記録媒体の欠陥数及び欠
陥長を求め、得られた結果に基づいて、記録を終了する
か、あるいは異なる領域に再度記録を行うかを決定する
ことを特徴とする請求項1記載の光磁気記録方法。2. A constant threshold value is provided for the sum signal, and a section where the monitored sum signal exceeds the threshold value is defined as a defect section, and a pulse width corresponding to the section is measured by a clock. The number of defects and the defect length of the magneto-optical recording medium are obtained in this way, and whether to end the recording or to perform the recording again in a different area is determined based on the obtained result. The described magneto-optical recording method.
とともに記録パワーを一定に保ったレーザ光を照射して
記録を行う磁界変調方式による光磁気記録方法におい
て、記録動作中に、光磁気記録媒体からの反射回折光を
2分割フォトダイオードを介して取り出した信号から得
た差信号をモニターし、その結果に基づいて、記録を終
了するか、あるいは記録条件を変更して再度記録を行う
かを決定することを特徴とする光磁気記録方法。3. A magneto-optical recording method according to a magnetic field modulation method, wherein a modulated magnetic field is applied to a magneto-optical recording medium and recording is performed by irradiating a laser beam whose recording power is kept constant. Monitor the difference signal obtained from the signal obtained by extracting the reflected diffracted light from the medium through the two-division photodiode, and based on the result, stop recording or change the recording conditions and perform recording again. A magneto-optical recording method characterized by:
おき、モニターした差信号が該しきい値を越えた時に記
録レーザパワーを上げることにより再度記録を行うこと
を特徴とする請求項3記載の光磁気記録方法。4. A recording apparatus is characterized in that a constant threshold value is set for the difference signal, and when the monitored difference signal exceeds the threshold value, recording laser power is increased to perform recording again. Item 3. The magneto-optical recording method according to Item 3.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP18037392A JP3273376B2 (en) | 1992-06-15 | 1992-06-15 | Magneto-optical recording method |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP18037392A JP3273376B2 (en) | 1992-06-15 | 1992-06-15 | Magneto-optical recording method |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH05347042A true JPH05347042A (en) | 1993-12-27 |
JP3273376B2 JP3273376B2 (en) | 2002-04-08 |
Family
ID=16082111
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP18037392A Expired - Fee Related JP3273376B2 (en) | 1992-06-15 | 1992-06-15 | Magneto-optical recording method |
Country Status (1)
Country | Link |
---|---|
JP (1) | JP3273376B2 (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH08221911A (en) * | 1995-02-16 | 1996-08-30 | Nec Corp | Magnetooptical disk recording device |
-
1992
- 1992-06-15 JP JP18037392A patent/JP3273376B2/en not_active Expired - Fee Related
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH08221911A (en) * | 1995-02-16 | 1996-08-30 | Nec Corp | Magnetooptical disk recording device |
Also Published As
Publication number | Publication date |
---|---|
JP3273376B2 (en) | 2002-04-08 |
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