JPH06267076A - Method for recording/reproducing optical data - Google Patents

Method for recording/reproducing optical data

Info

Publication number
JPH06267076A
JPH06267076A JP6009112A JP911294A JPH06267076A JP H06267076 A JPH06267076 A JP H06267076A JP 6009112 A JP6009112 A JP 6009112A JP 911294 A JP911294 A JP 911294A JP H06267076 A JPH06267076 A JP H06267076A
Authority
JP
Japan
Prior art keywords
semiconductor laser
recording
information
laser
high frequency
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
JP6009112A
Other languages
Japanese (ja)
Other versions
JP2638465B2 (en
Inventor
Toshimitsu Kaku
敏光 賀来
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.)
Hitachi Ltd
Original Assignee
Hitachi Ltd
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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP6009112A priority Critical patent/JP2638465B2/en
Publication of JPH06267076A publication Critical patent/JPH06267076A/en
Application granted granted Critical
Publication of JP2638465B2 publication Critical patent/JP2638465B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Optical Recording Or Reproduction (AREA)
  • Optical Head (AREA)

Abstract

PURPOSE:To obtain a laser driving apparatus which is effective not only when data is reproduced, but when data is recorded and deleted. CONSTITUTION:The apparatus uses a semiconductor laser 1 and a high frequency oscillator 22. The semiconductor laser 1 is driven by the high frequency oscillator 22, whereby laser noises generated from the semiconductor laser 1 are reduced. Driving of the high frequency oscillator 22 is stopped when the semiconductor laser is driven with high output pulses, for example, when data is recorded or deleted.

Description

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

【0001】[0001]

【産業上の利用分野】本発明は半導体レーザのレーザノ
イズを低減する高周波発振器を用いた半導体レーザの駆
動装置に係り、特に記録や消去などの半導体レーザのパ
ルス発振時の半導体レーザ駆動装置に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a semiconductor laser driving device using a high frequency oscillator for reducing laser noise of the semiconductor laser, and more particularly to a semiconductor laser driving device at the time of pulse oscillation of the semiconductor laser for recording and erasing.

【0002】[0002]

【従来の技術】半導体レーザは光デイスク,光プリンタ
等の光学的情報処理装置用の光源として多く利用されて
いる。近年,半導体レーザの横モード制御技術が発達し
て基本横モード発振し、かつ均一縦モード発振するもの
が多くなってきた。しかし、これにより可干渉性が良く
なり、逆に装置に組み込んだ場合、光学部品端面やデイ
スク面などから半導体レーザから出射した光が反射して
再びレーザにもどってくる時にフィードバックノイズと
いうが発生するという問題が生じてきた。
2. Description of the Related Art Semiconductor lasers are widely used as light sources for optical information processing devices such as optical discs and optical printers. In recent years, the lateral mode control technology for semiconductor lasers has been developed, and the number of those that perform fundamental transverse mode oscillation and uniform longitudinal mode oscillation has increased. However, this improves coherence, and conversely, when incorporated in a device, feedback noise occurs when the light emitted from the semiconductor laser is reflected from the end surface of the optical component or the disk surface and returns to the laser again. The problem has arisen.

【0003】このノイズは可干渉性の良い光が出射光と
反射光で干渉して、レーザの発振縦モードが、ジヤンプ
したり、多重縦モード発振したりして不安定になること
に帰因している。また発振縦モードの不安定は温度変化
によっても誘起される。すなわち温度変化により、単一
縦モード発振の波長はシフトし、連続的にシフトするだ
けでなく、離散的にジヤンプしてシフトする。このモー
ドジヤンプの際にノイズが発生する。これらノイズは光
通信や光デイスクにおいて、信号のS/Nを劣化させる
原因となる。
This noise is due to the fact that the light with good coherence interferes with the emitted light and the reflected light, and the oscillation longitudinal mode of the laser becomes unstable due to jumping or multiple longitudinal mode oscillation. is doing. Instability of the oscillation longitudinal mode is also induced by temperature changes. That is, the wavelength of the single longitudinal mode oscillation shifts due to the temperature change and not only shifts continuously but also jumps discretely and shifts. Noise is generated during this mode jump. These noises cause deterioration of signal S / N in optical communication and optical disks.

【0004】これらノイズを低減する方法として特公昭
59−9086号記載のように、レーザ駆動回路に高周波発振
器を設けてレーザを高周波変調によるものが考えられて
いる。しかし、この方法は連続的に高周波変調を行うD
C駆動の場合の場合についてレーザノイズを低減するこ
とのみが目的であった。
As a method for reducing these noises, Japanese Patent Publication Sho
As described in No. 59-9086, it is considered that a laser driving circuit is provided with a high frequency oscillator and the laser is modulated by high frequency. However, this method is a continuous D
The purpose was only to reduce laser noise in the case of C drive.

【0005】[0005]

【発明が解決しようとする課題】本発明は情報の再生時
のみでなく、情報の記録および消去時にも有効なレーザ
駆動装置を提供することにある。
SUMMARY OF THE INVENTION It is an object of the present invention to provide a laser driving device which is effective not only when reproducing information but also when recording and erasing information.

【0006】[0006]

【課題を解決するための手段】本発明の基本的な考え方
は再生時のみ高周波駆動し、記録モード,消去モード時
には高周波駆動を休止することである。
The basic idea of the present invention is to drive at high frequency only during reproduction, and stop at high frequency during recording and erasing modes.

【0007】[0007]

【作用】半導体レーザは、定格最大出力で記録・消去を
しており、この状態で高周波重量を行うと定格出力を越
えてしまい、レーザ自身の寿命に悪影響を与えるので、
本発明は、記録モード,消去モード時には高周波駆動を
休止させるのである。
[Operation] The semiconductor laser records and erases at the maximum rated output, and if the high frequency weight is applied in this state, the rated output will be exceeded and the life of the laser itself will be adversely affected.
According to the present invention, the high frequency drive is stopped in the recording mode and the erasing mode.

【0008】[0008]

【実施例】以下、本発明の一実施例を図1により説明す
る。これは光磁気デイスク装置に応用した場合であり、
半導体レーザ1から出た光はカツプリングレンズ7で集
光され、平行光となってビームスプリツク8,ガルバノ
ミラー9,絞り込みレンズ10を通って、光磁気記録膜
が形成してあるデイスク11上に1μm程度のスポツト
として絞り込まれる。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the present invention will be described below with reference to FIG. This is the case when applied to a magneto-optical disk device,
The light emitted from the semiconductor laser 1 is condensed by the coupling lens 7, becomes parallel light, passes through the beam split 8, the galvano mirror 9, and the focusing lens 10, and is placed on the disk 11 on which the magneto-optical recording film is formed. The spot size is about 1 μm.

【0009】光磁気記録膜としては遷移金属と希土類金
属のアモルファス化合物、たとえばTb−Fe,Tb−
Fe−Coなどがあり、面に垂直方向に磁化が配向した
垂直磁化膜となっている。この膜に高出力のレーザ光を
照射すると熱が発生して温度が上昇し、キューリ温度ま
で到達すると磁化がなくなる。この時に外部磁場として
電磁コイル12で磁場を印加すると温度上昇した部分だ
けがその方向に磁化が向き、まわりの磁化方向と反対の
時情報の記録が実行され、まわりの磁化方向と同一の時
は情報の消去が実行される。また信号再生は磁化の方向
によって膜に入射した直線偏光が反射する時に旋光角が
事なるカー(Kerr)効果を利用する。旋光角をθKとす
る時、例えば磁化の上向きに対して+θKだとすれば、
下向きに対しては−θKとなる。この旋光角はカー回転
角とよばれ、記録膜の組成やデイスク構造によつて異な
るが0.35度程度を非常に小さなものである。この信
号成分となるカー回転角はデイスク11から反射した光
に含まれ、絞れ込みレンズ10,ガルバーノミラー9を
通ってビームスプリツタ8で光路を分離された後、レン
ズ13を通りビームスプリツタ14でサーボ系と信号検
出系へ分離される。サーボ系はレンズ15と光検出器1
6で構成されており、従来良く知られているAF系は非
点収差法、TR系は回折差動法で光スポツトをデイスク
上に位置付ける(駆動回路は図示しない)。
The magneto-optical recording film is an amorphous compound of a transition metal and a rare earth metal, such as Tb-Fe or Tb-.
Fe-Co and the like are used, and the film is a perpendicular magnetic film in which the magnetization is oriented in the direction perpendicular to the plane. When this film is irradiated with a high-power laser beam, heat is generated and the temperature rises, and when it reaches the Curie temperature, the magnetization disappears. At this time, when a magnetic field is applied by the electromagnetic coil 12 as an external magnetic field, only the portion where the temperature rises is magnetized in that direction, and information recording is executed when it is opposite to the surrounding magnetization direction. Information is erased. In addition, signal reproduction utilizes the Kerr effect in which the angle of optical rotation changes when linearly polarized light incident on the film is reflected depending on the direction of magnetization. When the rotation angle is θ K , for example, if it is + θ K with respect to the upward magnetization,
For downward, it becomes −θ K. This optical rotation angle is called the Kerr rotation angle, and although it depends on the composition of the recording film and the disk structure, it is as small as about 0.35 degree. The Kerr rotation angle, which is the signal component, is included in the light reflected from the disk 11, passes through the focusing lens 10 and the galvanometer mirror 9, and the optical path is separated by the beam splitter 8, and then passes through the lens 13 and the beam splitter. At 14, the servo system and the signal detection system are separated. Servo system is lens 15 and photo detector 1
The AF system, which is well known in the art, positions the optical spot on the disk by the astigmatism method and the TR system by the diffraction differential method (the drive circuit is not shown).

【0010】信号検出系はλ/2板17(λは半導体レ
ーザ波長)、偏光ビームスプリツタ18で光量を2等分
して光検出器19,20の出力を差動増幅器23で差動
する差動方式をとり、光磁気信号が得られる。この方式
はレーザノイズやデイスクノイズなどの非量変動に起因
するノイズは低減できる効果を有している。また2つの
光検出器19,20の出力の和は加算器24で得られ、
これはデイスクの反射光量を検出するのでデイスク上に
あらかじめ凹凸の形で記録されている番地情報などの検
出に用いる。検出された光磁気信号と番地情報信号はコ
ントローラ5へ入力される。
In the signal detection system, a λ / 2 plate 17 (λ is a semiconductor laser wavelength) and a polarization beam splitter 18 divide the light quantity into two equal parts, and the outputs of the photodetectors 19 and 20 are differentiated by a differential amplifier 23. A differential method is used to obtain a magneto-optical signal. This method has an effect of reducing noises caused by non-quantity fluctuations such as laser noises and disk noises. The sum of the outputs of the two photodetectors 19 and 20 is obtained by the adder 24,
Since this detects the amount of reflected light from the disk, it is used to detect the address information or the like that has been recorded beforehand in the form of unevenness on the disk. The detected magneto-optical signal and address information signal are input to the controller 5.

【0011】図2を用いてコントローラ5の構成及び動
作について説明する。差動増幅器23から得られる光磁
気信号と加算器24から得られる番地情報信号はアナロ
グスイツチ51において、番地情報信号を入力したマー
ク検出回路52からのタイミングを用いて切換え、番地
情報付の情報信号となる。この情報信号はパルス化回路
53でデイジタル化され、復調回路55において読取り
のタイミングクロツクを発生するVFO(Variable Fre
quency Oscillator)回路54からのクロツクをもとに
情報データと番地データが読取られ、マイクロプロセッ
サ56へ入力され認識される。次にマイクロプロセッサ
56から送出される情報データと番地データは変調回路
57でタイミングを合わせた後、変調(たとえば2−7
変調)され、自動パワー制御回路6に入力される。ま
た、装置のシーケンスを司るシーケンス回路58はマイ
クロプロセツサ56からの命令により記録,再生,消去
のモード信号を発生し、レーザの駆動信号発生と自動パ
ワー制御を行う自動パワー制御回路6とレーザの駆動回
路2に設けられた高周波発振回路22へ入力される。自
動パワー制御回路6は駆動回路2に対してレーザの駆動
信号(DC+パルス駆動)の送出と半導体レーザ1のモ
ニタ用光検出器からの制御信号を受けて自動パワー制御
を行う。
The configuration and operation of the controller 5 will be described with reference to FIG. The magneto-optical signal obtained from the differential amplifier 23 and the address information signal obtained from the adder 24 are switched in the analog switch 51 by using the timing from the mark detection circuit 52 to which the address information signal is input, and the information signal with the address information is added. Becomes This information signal is digitized by the pulse conversion circuit 53, and a VFO (Variable Fres) which generates a read timing clock in the demodulation circuit 55.
Based on the clock from the quency oscillator circuit 54, information data and address data are read and input to the microprocessor 56 for recognition. Then, the information data and the address data sent from the microprocessor 56 are timed by the modulation circuit 57 and then modulated (for example, 2-7).
It is modulated and input to the automatic power control circuit 6. A sequence circuit 58, which controls the sequence of the apparatus, generates a mode signal for recording, reproduction, and erasing in response to a command from the microprocessor 56, and generates the drive signal of the laser and the automatic power control circuit 6 for performing automatic power control. It is input to the high frequency oscillation circuit 22 provided in the drive circuit 2. The automatic power control circuit 6 sends a laser drive signal (DC + pulse drive) to the drive circuit 2 and receives a control signal from the monitor photodetector of the semiconductor laser 1 to perform automatic power control.

【0012】次に半導体レーザの高周波駆動について図
3により説明する。半導体レーザ1は駆動回路2で駆動
される。半導体レーザ1内にレーザチツプ3,モニタ用
光検出器4から成っており、レーザチツプ3は駆動ライ
ン31に、モニタ用光検出器4は検出ライン41に接続
されている。駆動回路2はレーザチツプ3を通常駆動す
るドライバアンプ21と高周波発振回路22から成って
おり、ドライバアンプ21の出力線と高周波発振回路2
2の出力線はコンデンサCを通して直結されて駆動ライ
ン31となる。ドライバアンプ21は上位コントローラ
5から記録,消去時はパルスが送出され、それに応じて
パルス発振をする。
Next, high frequency driving of the semiconductor laser will be described with reference to FIG. The semiconductor laser 1 is driven by the drive circuit 2. The semiconductor laser 1 comprises a laser chip 3 and a photodetector 4 for monitoring. The laser chip 3 is connected to a drive line 31 and the photodetector 4 for monitoring is connected to a detection line 41. The drive circuit 2 includes a driver amplifier 21 that normally drives the laser chip 3 and a high frequency oscillation circuit 22, and the output line of the driver amplifier 21 and the high frequency oscillation circuit 2
The second output line is directly connected to the drive line 31 through the capacitor C. The driver amplifier 21 sends a pulse from the host controller 5 during recording and erasing, and oscillates the pulse in response to the pulse.

【0013】図4,図5を用いて光磁気デイスクにおけ
る記録モード,再生モードおよび消去モードについて説
明する。図4は各モード時の波形を表わす。(A)は再
生モードでありモード信号aは“L”のまま、情報デー
タ信号bは“L”のまま、ドライバアンプ出力CはIR
(mA)、高周波発振回路出力dはONのまま、レーザ
駆動電流波形eはドライバアンプ出力Cと高周波発振回
路出力dを加算したものとなつており、連続的に高周波
重量を行う。(B)は記録モードであり、モード信号a
はセクタ単位の記録を行うためにセクタ毎に“H”とな
り、情報データ信号bはセクタ期間データパルスが発生
し、ドライバ出力Cは再生時の電流IRに情報データ分
Wが重畳された波形となり、高周波発振器出力dはモ
ード信号a(セクタ毎にON)によつてモード信号aが
“L”の時のみに発振する波形となり、レーザ駆動波形
eはドライバ出力Cと高周波発振器出力dを加算したも
のとなり、セクタ間のヘツダー信号を読取る時のみ高周
波重量をすることになる。(C)は消去モードであり、
(B)の記録モード時に比べて情報データbはデータパ
ルスがなくセクタ中“H”となっているだけで、他の動
作は同様である。
A recording mode, a reproducing mode and an erasing mode in the magneto-optical disk will be described with reference to FIGS. FIG. 4 shows the waveform in each mode. (A) is a reproduction mode, the mode signal a remains "L", the information data signal b remains "L", and the driver amplifier output C is IR.
(MA), the high frequency oscillation circuit output d remains ON, the laser drive current waveform e is the sum of the driver amplifier output C and the high frequency oscillation circuit output d, and high frequency weighting is performed continuously. (B) is the recording mode, and the mode signal a
Becomes "H" for each sector to perform recording in sector units, a data pulse is generated in the information data signal b during the sector period, and the driver output C has the information data I W superimposed on the reproduction current I R. The high frequency oscillator output d becomes a waveform which oscillates only when the mode signal a is "L" by the mode signal a (ON for each sector), and the laser drive waveform e shows the driver output C and the high frequency oscillator output d. It becomes the sum, and the high frequency weight is added only when the header signal between the sectors is read. (C) is an erase mode,
Compared with the recording mode of (B), the information data b has no data pulse and is "H" in the sector, and other operations are the same.

【0014】図5は各モードにおけるレーザ駆動状態を
示し、図4の参考図である。また図6に高周波発振回路
22の基本例を示す。モニタ用光検出器4からの検出ラ
イン41はレーザパワーの自動パワー制御回路6に導か
れ、検出した制御信号を用いてドライバアンプ21を制
御し、パワーコントロールを行う。
FIG. 5 shows a laser driving state in each mode and is a reference diagram of FIG. Further, FIG. 6 shows a basic example of the high frequency oscillation circuit 22. The detection line 41 from the monitor photodetector 4 is guided to the laser power automatic power control circuit 6 and controls the driver amplifier 21 using the detected control signal to perform power control.

【0015】本発明を日立製半導体レーザHL−8314E
形(830nm,30mW出力)を用いて確認した結
果、再生時には相対雑音レベルRIN値で2桁程度低減
でき、また記録,消去時ら高周波重量を休止しても記録
データにエラーが発生しないことがわかった。この時高
周波発振周波数は600MHzであり、電流変調度は14
0〜160%であつた。
According to the present invention, a semiconductor laser HL-8314E manufactured by Hitachi is used.
As a result of confirming using the shape (830 nm, 30 mW output), it is possible to reduce the relative noise level RIN value by about 2 digits at the time of reproduction, and no error occurs in the recorded data even when the high frequency weight is stopped at the time of recording and erasing. all right. At this time, the high frequency oscillation frequency is 600 MHz and the current modulation degree is 14
It was 0 to 160%.

【0016】[0016]

【発明の効果】以上の如く、本発明によれば、記録,再
生,消去時の高周波重量を制御することにより、記録,
再生,消去時のレーザノイズを低減できる効果がある。
As described above, according to the present invention, by controlling the high frequency weight during recording, reproduction and erasing, recording,
This has the effect of reducing laser noise during playback and erasing.

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

【図1】本発明の実施例を説明するための図。FIG. 1 is a diagram for explaining an embodiment of the present invention.

【図2】本発明の実施例を説明するための図。FIG. 2 is a diagram for explaining an embodiment of the present invention.

【図3】本発明の実施例を説明するための図。FIG. 3 is a diagram for explaining an example of the present invention.

【図4】本発明の実施例を説明するための図。FIG. 4 is a diagram for explaining an example of the present invention.

【図5】本発明の実施例を説明するための図。FIG. 5 is a diagram for explaining an example of the present invention.

【図6】本発明の実施例を説明するための図。FIG. 6 is a diagram for explaining an example of the present invention.

【符号の説明】[Explanation of symbols]

1…半導体レーザ、2…駆動回路、3…レーザチツプ、
4…モニタ用光検出器、5…コントローラ、6…自動パ
ワー制御回路、22…高周波発振回路。
1 ... Semiconductor laser, 2 ... Driving circuit, 3 ... Laser chip,
4 ... Photodetector for monitor, 5 ... Controller, 6 ... Automatic power control circuit, 22 ... High frequency oscillation circuit.

Claims (4)

【特許請求の範囲】[Claims] 【請求項1】高周波の重畳によって半導体レーザの駆動
を制御し、上記半導体レーザの出射光を記録媒体上に照
射し、情報の記録又は再生を行なう光学的情報記録再生
方法において、上記記録の際に上記高周波の重畳を停止
することを特徴とする光学的情報記録再生方法。
1. An optical information recording / reproducing method in which driving of a semiconductor laser is controlled by superposition of high frequencies, and light emitted from the semiconductor laser is irradiated onto a recording medium to record or reproduce information. An optical information recording / reproducing method, characterized in that the superposition of the high frequencies is stopped.
【請求項2】高周波の重畳によって半導体レーザの駆動
を制御し、上記半導体レーザの出射光を記録媒体上に照
射し、情報の記録又は消去を行なう光学的情報記録再生
方法において、上記消去の際に上記高周波の重畳を停止
することを特徴とする光学的情報記録再生方法。
2. An optical information recording / reproducing method for recording or erasing information by controlling driving of a semiconductor laser by superimposing a high frequency and irradiating a recording medium with light emitted from the semiconductor laser. An optical information recording / reproducing method, characterized in that the superposition of the high frequencies is stopped.
【請求項3】半導体レーザからのレーザ光を記録すべき
情報に応じて変調して記録媒体に照射することにより情
報を記録し、半導体レーザからのレーザ光を情報の記録
された媒体に照射して戻ってくる光から当該情報を再生
する光学的情報記録再生方法において、情報再生時のみ
上記半導体レーザに高周波を印加することを特徴とする
光学的情報記録再生方法。
3. Information is recorded by modulating laser light from a semiconductor laser according to the information to be recorded and irradiating the recording medium, and irradiating the medium on which the information is recorded with the laser light from the semiconductor laser. In the optical information recording / reproducing method for reproducing the information from the returning light, a high frequency is applied to the semiconductor laser only when reproducing the information.
【請求項4】半導体レーザからのレーザ光を第1の所定
レベルで情報の記録された媒体に照射して戻ってくる光
から当該情報を再生し、半導体レーザからのレーザ光を
上記第1のレベルよりも高い第2のレベルで記録媒体に
照射して情報を記録または消去する光学的情報記録再生
方法において、上記半導体レーザが上記第1のレベルで
駆動されている場合半導体レーザに一定周波数の駆動信
号を印加し、上記第2のレベルで駆動されている場合上
記駆動信号の印加を停止することを特徴とする光学的情
報記録再生方法。
4. A laser beam from a semiconductor laser is irradiated onto a medium on which information is recorded at a first predetermined level and the information is reproduced from the returning light, and the laser beam from the semiconductor laser is converted into the first beam. In an optical information recording / reproducing method of irradiating a recording medium at a second level higher than the level to record or erase information, when the semiconductor laser is driven at the first level, An optical information recording / reproducing method, characterized in that a drive signal is applied and when the drive is performed at the second level, the application of the drive signal is stopped.
JP6009112A 1994-01-31 1994-01-31 Optical information recording / reproducing method Expired - Lifetime JP2638465B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6009112A JP2638465B2 (en) 1994-01-31 1994-01-31 Optical information recording / reproducing method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6009112A JP2638465B2 (en) 1994-01-31 1994-01-31 Optical information recording / reproducing method

Related Parent Applications (1)

Application Number Title Priority Date Filing Date
JP60258534A Division JP2528821B2 (en) 1985-11-20 1985-11-20 Optical information processing device

Publications (2)

Publication Number Publication Date
JPH06267076A true JPH06267076A (en) 1994-09-22
JP2638465B2 JP2638465B2 (en) 1997-08-06

Family

ID=11711557

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6009112A Expired - Lifetime JP2638465B2 (en) 1994-01-31 1994-01-31 Optical information recording / reproducing method

Country Status (1)

Country Link
JP (1) JP2638465B2 (en)

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61192043A (en) * 1985-02-20 1986-08-26 Sharp Corp Semiconductor laser driving device

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61192043A (en) * 1985-02-20 1986-08-26 Sharp Corp Semiconductor laser driving device

Also Published As

Publication number Publication date
JP2638465B2 (en) 1997-08-06

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