JP2528821B2 - Optical information processing device - Google Patents

Optical information processing device

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Publication number
JP2528821B2
JP2528821B2 JP60258534A JP25853485A JP2528821B2 JP 2528821 B2 JP2528821 B2 JP 2528821B2 JP 60258534 A JP60258534 A JP 60258534A JP 25853485 A JP25853485 A JP 25853485A JP 2528821 B2 JP2528821 B2 JP 2528821B2
Authority
JP
Japan
Prior art keywords
semiconductor laser
recording
mode signal
erasing
optical
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
JP60258534A
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Japanese (ja)
Other versions
JPS62119743A (en
Inventor
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
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Application filed by Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP60258534A priority Critical patent/JP2528821B2/en
Priority to US06/932,495 priority patent/US4819242A/en
Publication of JPS62119743A publication Critical patent/JPS62119743A/en
Application granted granted Critical
Publication of JP2528821B2 publication Critical patent/JP2528821B2/en
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Expired - Lifetime legal-status Critical Current

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  • Semiconductor Lasers (AREA)

Description

【発明の詳細な説明】 〔発明の利用分野〕 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。
Description: 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 a semiconductor laser, and particularly to a semiconductor laser pulse oscillation such as recording or erasing. The present invention relates to a semiconductor laser drive device.

〔発明の背景〕[Background of the Invention]

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つて
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
もどつてくる時にフイードバツクノイズというが発生す
るという問題が生じてきた。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つても誘起される。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。
Semiconductor lasers are often used as light sources for optical information processing devices such as optical disks and optical printers. recent years,
Lateral mode control technology for semiconductor lasers has been developed, and many of them have a fundamental lateral mode oscillation and a uniform longitudinal mode oscillation. However, this improves the coherence, and conversely, when it is incorporated into the device, 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, it is called feedback noise. The problem of occurring has arisen. 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. . Instability of the oscillation longitudinal mode is also induced by temperature change. That is, the wavelength of the single longitudinal mode oscillation shifts due to a temperature change, and not only continuously shifts, but also discretely jumps and shifts. Noise occurs during this mode jump. These noises are signal S / N in optical communication and optical disk.
Cause deterioration.

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DC駆動の場合
についてレーザノイズを低減することのみが目的であつ
た。
As a method for reducing these noises, as disclosed in Japanese Examined Patent Publication No. 59-9086, it is considered that a laser driving circuit is provided with a high-frequency oscillator and the laser is subjected to high-frequency modulation. However, this method was only intended to reduce the laser noise in the case of DC drive in which continuous high frequency modulation is performed.

〔発明の目的〕[Object of the Invention]

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。
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.

〔発明の概要〕[Outline of Invention]

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。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
超えてしまい、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。
The basic idea of the present invention is to drive at high frequency only during playback,
High-frequency driving is stopped in the recording mode and the erasing mode. The semiconductor laser performs recording / erasing at the rated maximum 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. Sometimes the high frequency drive is stopped.

〔発明の実施例〕Example of Invention

以下、本発明の一実施例を第1図により説明する。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、平行光となつ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を通つて、光磁気記録膜を形成して
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。光磁気記録膜としては遷移金属と希土類金属の
アモルフアス化合物、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つて
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、キユ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つて膜に入射した
直線偏光が反射する時に旋光角が異なるカー(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度程点を非常に
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を通つ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16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)。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
イズなどの光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。
An embodiment of the present invention will be described below with reference to FIG. This is a case where it is applied to a magneto-optical disk device, in which the light emitted from the semiconductor laser 1 is condensed by a coupling lens 7 and collimated into a beam split 8 and a galvano mirror.
9, After passing through the aperture lens 10, the aperture is focused as a spot of about 1 μm on the disk 11 on which the magneto-optical recording film is formed. As the magneto-optical recording film, there are amorphous compounds of transition metals and rare earth metals, such as Tb-Fe and Tb-Fe-Co, which form a perpendicular magnetic film in which the magnetization is oriented in the direction perpendicular to the plane. When this film is irradiated with high-power laser light, heat is generated and the temperature rises, and when the temperature reaches the Curie temperature, the magnetization disappears. At this time, when a magnetic field is applied as an external magnetic field by the electromagnetic coil 12, only the temperature-increased portion is magnetized in that direction, and information recording is executed when the magnetization direction is opposite to the surrounding magnetization direction. Information is erased. The signal reproduction utilizes the Kerr effect in which the angle of optical rotation is different when the linearly polarized light incident on the film is reflected depending on the direction of magnetization. When the optical rotation angle is θ K , for example, if it is + θ K for upward magnetization, −θ K for downward magnetization.
Becomes This optical rotation angle is called the Kerr rotation angle, and although it differs depending on the composition of the recording film and the disk structure, it has a very small point of about 0.35 degrees. The Kerr rotation angle that is this signal component is included in the light reflected from the disk 11, and the focusing lens 10,
After passing through the galvanometer mirror 9, the beam splitter 8 separates the optical path, and then passes through the lens 13 and the beam splitter 14 separates the optical system into a servo system and a signal detection system. Servo system is a lens
It is composed of 15 and photodetector 16. The AF system, which is well known in the past, uses the astigmatism method, and the TR system uses the diffraction differential method to position the optical spot on the disk (the drive circuit is not shown). The signal detection system is a λ / 2 plate 17 (λ is a semiconductor laser wavelength), a polarization beam splitter 18 divides the light amount into two equal parts, and the output of the photodetectors 19 and 20 is differentially differentiated by a differential amplifier 23. Then, a magneto-optical signal is obtained. This method has an effect of reducing noise such as laser noise and disk noise caused by fluctuations in light amount. The sum of the outputs of the two photodetectors 19 and 20 is obtained by an adder 24, which detects the reflected light amount of the disk, and is used for detecting the address information or the like which is 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.

第2図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 Frequency 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、マイクロプロセツサ56へ入力され認識される。
次にマイクロプロセツサ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信回路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 analog switches 51.
In the above, the address signal is switched 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 obtained. This information signal is digitized by the pulse conversion circuit 53, and a VFO (Variable Frequency Oscillator) circuit for generating a read timing clock in the demodulation circuit 55.
The information data and address data are read based on the clock from 54 and input to the microprocessor 56 for recognition.
Next, the information data and the address data sent from the microprocessor 56 are modulated (for example, 2-7 modulated) after the timing is adjusted by the modulation circuit 57, and the automatic power control circuit 6
Is input to A sequence circuit 58, which controls the sequence of the apparatus, generates a mode signal for recording, reproducing, and erasing in response to a command from the microprocessor 56, generates an automatic power control circuit 6 for performing laser drive signal generation and automatic power control, and a laser It is input to the high-frequency transmission 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 monitoring photodetector of the semiconductor laser 1 to perform automatic power control.

次に半導体レーザの高周波駆動について第3図により
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
から成つており、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から成つており、ドライバアン
プ21の出力線と高周波発振回路22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。第4図,
第5図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。第4図は
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、レーザ駆動電流波長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IWが重量された波長とな
り、高周波発振器出力dはモード信号a(セクタ毎にO
N)によつてモード信号aが“L"の時のみに発振する波
長となり、レーザ駆動波長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
なつているだけで、他の動作は同様である。
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.
Laser chip 3 in semiconductor laser 1 and photo detector 4 for monitoring
The laser chip 3 is connected to the drive line 31, and the monitoring photodetector 4 is connected to the detection line 41. The drive circuit 2 is composed of 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 output line of the high frequency oscillation circuit 22 are directly connected through a capacitor C to form a drive line 31. The driver amplifier 21 outputs a pulse from the host controller 5 during recording and erasing, and oscillates the pulse in response to the pulse. Figure 4,
A recording mode, a reproducing mode and an erasing mode in the magneto-optical disk will be described with reference to FIG. FIG. 4 shows the waveform in each mode. (A) remains in is the mode signal a "L" playback mode, while the information data signals b is "L", the driver amplifier output C is I R (mA), high-frequency oscillator output d remains turned ON, The laser drive current wavelength e is the sum of the driver amplifier output C and the high frequency oscillation circuit output d, and the high frequency weight is continuously performed. (B) is a recording mode, the mode signal a becomes "H" for each sector for recording in sector units, the information data signal b generates a data pulse in the sector period, and the driver output C shows the current during reproduction. The wavelength becomes the weight of I R by the information data I W , and the high frequency oscillator output d outputs the mode signal a (O for each sector.
N) makes the wavelength oscillate only when the mode signal a is “L”, and the laser drive wavelength e is the sum of the driver output C and the high frequency oscillator output d. It will be heavy.
(C) is an erasing mode, the information data b has no data pulse and is "H" in the sector as compared with the recording mode of (B), and other operations are the same.

第5図は各モードにおけるレーザ駆動状態を示し、第
4図の参考図である。また第6図に高周波発振回路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. FIG. 6 shows a basic example of the high frequency oscillation circuit 22. Detection line 41 from the photodetector 4 for monitor
Is guided to the automatic power control circuit 6 for laser power, and controls the driver amplifier 21 using the detected control signal to perform power control.

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
とがわかつた。この時高周波発振周波数は60MHzであ
り、電流変調度は140〜160%であつた。
The present invention is based on the Hitachi semiconductor laser HL-8314E (830nm, 30mW
As a result of confirmation using the output), it was found that the relative noise level RIN value could be reduced by about two digits during reproduction, and that no error occurred in the recorded data even when the high frequency weight was stopped during recording and erasing. At this time, the high frequency oscillation frequency was 60 MHz and the current modulation degree was 140 to 160%.

〔発明の効果〕〔The invention's effect〕

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 at the time of recording, reproducing and erasing, there is an effect that the laser noise at the time of recording, reproducing and erasing can be reduced.

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

第1図〜第6図は本発明の実施例を説明するための図で
ある。 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 to 6 are views for explaining an embodiment of the present invention. 1 ... Semiconductor laser, 2 ... Drive circuit, 3 ... Laser chip, 4 ... Monitor photodetector, 5 ... Controller,
6 ... Automatic power control circuit, 22 ... High frequency oscillation circuit.

Claims (2)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】半導体レーザと、該半導体レーザを駆動す
る駆動手段と、該駆動手段を制御する制御手段と、上記
半導体レーザの出射光を記録媒体上に導く光学系と、上
記記録媒体から戻る光を検出する光検出手段と、該光検
出手段の出力に基づいて信号を形成する信号再生系とを
有し、情報を光学的に記録および再生する光情報処理装
置において、上記駆動手段は、上記半導体レーザを変調
する変調手段及び、該変調手段と半導体レーザとの間に
コンデンサを介して接続される高周波発振手段とを有
し、上記制御手段は、情報の記録若しくは消去または再
生の状態を示すモード信号を得るモード信号形成手段を
有し、該モード信号が情報の記録若しくは消去を示す場
合、上記高周波発振手段による半導体レーザへの高周波
電流の印加を休止することを特徴とする光情報処理装
置。
1. A semiconductor laser, driving means for driving the semiconductor laser, control means for controlling the driving means, an optical system for guiding the emitted light of the semiconductor laser onto a recording medium, and returning from the recording medium. In an optical information processing apparatus which has a light detecting means for detecting light and a signal reproducing system for forming a signal based on the output of the light detecting means, and which optically records and reproduces information, the driving means comprises: The control means has a modulation means for modulating the semiconductor laser and a high-frequency oscillation means connected between the modulation means and the semiconductor laser via a capacitor, and the control means controls a state of recording, erasing or reproducing of information. When the mode signal forming means for obtaining the indicated mode signal is provided and the mode signal indicates recording or erasing of information, the application of the high frequency current to the semiconductor laser by the high frequency oscillating means is stopped. Optical information processing apparatus, characterized in that.
【請求項2】前記モード信号形成手段は情報の記録、再
生、消去の各状態を示すモード信号を発生するシーケン
ス回路であることを特徴とする特許請求の範囲第1項記
載の光情報処理装置。
2. The optical information processing apparatus according to claim 1, wherein the mode signal forming means is a sequence circuit for generating a mode signal indicating each of recording, reproducing and erasing states of information. .
JP60258534A 1985-11-20 1985-11-20 Optical information processing device Expired - Lifetime JP2528821B2 (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
JP60258534A JP2528821B2 (en) 1985-11-20 1985-11-20 Optical information processing device
US06/932,495 US4819242A (en) 1985-11-20 1986-11-20 Semiconductor laser driver circuit

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

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JP6009112A Division JP2638465B2 (en) 1994-01-31 1994-01-31 Optical information recording / reproducing method

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JPS62119743A JPS62119743A (en) 1987-06-01
JP2528821B2 true JP2528821B2 (en) 1996-08-28

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JP2526596Y2 (en) * 1986-03-04 1997-02-19 パイオニア株式会社 Optical information recording / reproducing device
JPH0610884B2 (en) * 1986-07-01 1994-02-09 日本電気株式会社 Optical pickup device
US5042022A (en) * 1986-07-31 1991-08-20 Sony Corporation Optical disk recording/reproducing apparatus with synchronized data writing
JP2635987B2 (en) * 1988-01-25 1997-07-30 キヤノン株式会社 Semiconductor laser driver
JPH02118927A (en) * 1988-10-27 1990-05-07 Canon Inc Method and device for driving semiconductor laser
JP2935268B2 (en) * 1989-09-07 1999-08-16 パイオニア株式会社 Optical power control circuit for semiconductor light emitting device
JP2525943B2 (en) * 1990-08-02 1996-08-21 富士通株式会社 Laser diode control system for optical recording / reproducing apparatus
US5495464A (en) * 1993-01-20 1996-02-27 Olympus Optical Co., Ltd. Optical data recording/reproducing apparatus
EP1936611B1 (en) 2005-10-04 2009-09-23 Panasonic Corporation Optical disc drive device and optical disc reproduction method using same
WO2007148669A1 (en) * 2006-06-20 2007-12-27 Pioneer Corporation Optical recording/reproducing method and system, and program

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JPS60170041A (en) * 1984-02-14 1985-09-03 Sharp Corp Optical pickup device

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