JPS61194649A - Optical recording and reproducing device - Google Patents
Optical recording and reproducing deviceInfo
- Publication number
- JPS61194649A JPS61194649A JP60034941A JP3494185A JPS61194649A JP S61194649 A JPS61194649 A JP S61194649A JP 60034941 A JP60034941 A JP 60034941A JP 3494185 A JP3494185 A JP 3494185A JP S61194649 A JPS61194649 A JP S61194649A
- Authority
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- Japan
- Prior art keywords
- current
- output
- circuit
- semiconductor laser
- recording
- 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.)
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- Optical Recording Or Reproduction (AREA)
- Optical Head (AREA)
- Semiconductor Lasers (AREA)
Abstract
Description
【発明の詳細な説明】
(概要〕
半導体レーザ駆動回路において、側路電流を切換え制御
することにより折点特性を有する半導体レーザの出力特
性の低出力領域にも対応できるようにするものである。DETAILED DESCRIPTION OF THE INVENTION (Summary) In a semiconductor laser drive circuit, by switching and controlling the bypass current, it is possible to cope with the low output region of the output characteristics of a semiconductor laser having corner characteristics.
本発明は光デイスク装置や光磁気ディスク装置等の光学
的記録再生装置に用いられる半導体レーデの駆動回路に
係り、特に情報の再生時および記録時における半導体レ
ーザの光出力の安定化を図る駆動回路の改良に関する。The present invention relates to a drive circuit for a semiconductor laser used in an optical recording/reproducing device such as an optical disk device or a magneto-optical disk device, and in particular a drive circuit for stabilizing the optical output of a semiconductor laser during information reproduction and recording. Regarding improvements.
すなわち、光学的記録再生装置には光源として半導体レ
ーザが広く用いられ、その出射光量はフォトダイオード
を利用した光量検知器で電流に変換してモニタされる。That is, semiconductor lasers are widely used as light sources in optical recording/reproducing devices, and the amount of emitted light is converted into electric current and monitored by a light amount detector using a photodiode.
再生時には光量検知器の出力を電圧変換して自動光量制
御回路(Auto Power Control 以
下APC回路と略称する)に負帰還して半導体レーザの
出射光量が一定値になるように再生電流が制御される。During playback, the output of the light intensity detector is converted into a voltage and fed back negatively to an automatic power control circuit (hereinafter abbreviated as APC circuit) to control the playback current so that the amount of light emitted by the semiconductor laser remains at a constant value. .
そして光学系の簡略化等により記録時にもこの半導体レ
ーザが利用される。記録するためには半導体レーザに前
記再生電流に記録電流を重畳する変調回路が用いられる
。This semiconductor laser is also used during recording due to the simplification of the optical system. For recording, a modulation circuit is used in the semiconductor laser to superimpose a recording current on the reproducing current.
しかしながら、記録電流を再生電流に重畳すると、光量
検知器の出力が変化するので、このままでは半導体レー
ザの出射光量を一定値にすべく作用するAPC回路と、
その一定値を重畳電流により増加させようとする変調回
路は両立しない矛盾があり、これを両立させる手段の開
発が望まれている。However, when the recording current is superimposed on the reproduction current, the output of the light amount detector changes, so if this is done, the APC circuit that acts to keep the amount of light emitted from the semiconductor laser at a constant value.
A modulation circuit that attempts to increase this constant value by using a superimposed current has an irreconcilable contradiction, and it is desired to develop a means for achieving both of these problems.
第4図は従来の半導体レーザ駆動回路のブロック図を示
す。図において、1は半導体レーザ、3は光量検知器で
あって通常フォトダイオード等が用いられ、半導体レー
ザ1と一体的に形成され、半導体レーザ1を駆動する電
流により出射される光出力の後方光を受光し、該光出力
の強度に対応した電流1pdを出力し半導体レーザ1の
レーザ光強度モニタとして利用される。FIG. 4 shows a block diagram of a conventional semiconductor laser drive circuit. In the figure, 1 is a semiconductor laser, and 3 is a light amount detector, which is usually a photodiode or the like, is formed integrally with the semiconductor laser 1, and is a rear light of the optical output emitted by the current that drives the semiconductor laser 1. It receives the light, outputs a current of 1 pd corresponding to the intensity of the light output, and is used as a laser light intensity monitor of the semiconductor laser 1.
第1図に示した駆動回路2は第4図では再生電流Ibを
出力するAPC回路21と、記録電流Iwを出力する変
調回路22とから構成され、変調回路22はスイッチン
グ回路221と定電流回路222とから構成されている
。The drive circuit 2 shown in FIG. 1 is composed of an APC circuit 21 that outputs a reproduction current Ib and a modulation circuit 22 that outputs a recording current Iw in FIG. 4, and the modulation circuit 22 includes a switching circuit 221 and a constant current circuit. 222.
4は抵抗であってこれに流れる光量検知器3の検出電流
1rを電圧に変換し、APC回路21にフィードバック
して閉ループ回路5を構成する。−Vは印加された電源
電圧を示す。Reference numeral 4 denotes a resistor which converts the detection current 1r of the light amount detector 3 flowing through the resistor into a voltage and feeds it back to the APC circuit 21 to form a closed loop circuit 5. -V indicates the applied power supply voltage.
閉ループ回路5により光学的ディスク装置の光源用半導
体レーザlに情報を再生するための駆動電流rbを供給
する回路を構成し、APC回路21は再生時における半
導体レーザ1の光出力を常に一定値に維持するように再
生電流1bを制御する。The closed loop circuit 5 constitutes a circuit that supplies a drive current rb for reproducing information to the semiconductor laser l for the light source of the optical disc device, and the APC circuit 21 always keeps the optical output of the semiconductor laser 1 at a constant value during reproduction. The reproduction current 1b is controlled so as to maintain the reproduction current 1b.
221は高速のスイッチング回路、222は定電流回路
、Mは変調信号を示し、半導体レーザ1に流れる再生時
の駆動電流Tbに断続した記録電流Iwを重畳供給する
変調回路22を構成している。221 is a high-speed switching circuit, 222 is a constant current circuit, and M is a modulation signal, which constitutes a modulation circuit 22 that superimposes and supplies an intermittent recording current Iw to a drive current Tb flowing through the semiconductor laser 1 during reproduction.
通常APC回路21は帯域的に高域特性が良(ないので
高速変調が望めず、したがって図示するよ′うに再生時
の駆動電流1bを流すAPC回路21とは別に独立した
記録電流1w重畳用の変調回路22が半導体レーザ1に
並列に構成されている。Normally, the APC circuit 21 does not have good high-frequency characteristics in terms of band, so high-speed modulation cannot be expected. A modulation circuit 22 is configured in parallel to the semiconductor laser 1.
情報の再生時にはAPC回路21により所定の駆動電流
Tbを半導体レーザ1に流し、情報の記録時には変調信
号Mによって高速のスイッチング回路221を駆動し、
半導体レーザ1に断続した定電流の記録電流−を重畳し
Ib+1−を流す。When reproducing information, a predetermined drive current Tb is passed through the semiconductor laser 1 by the APC circuit 21, and when recording information, a high-speed switching circuit 221 is driven by the modulation signal M,
An intermittent constant recording current - is superimposed on the semiconductor laser 1 to flow Ib+1-.
但しこの場合APC回路21が単なるフィードバック回
路のままであると、記録電流Iwの重畳に対応して検出
電流Isも増加し抵抗4の検出するフィードバック量が
増加するため、APC回路21の出力はその平均値を情
報の再生時と同じレベルにするように作用して矛盾が発
生するので、これを解決するために記録時に対応する検
出電流Isを側路させる側路回路6とこれを駆動する減
衰器10が設けられている。However, in this case, if the APC circuit 21 remains a mere feedback circuit, the detection current Is will also increase in response to the superimposition of the recording current Iw, and the amount of feedback detected by the resistor 4 will increase, so the output of the APC circuit 21 will be Inconsistency occurs because the average value is made to be at the same level as when reproducing information, so in order to solve this problem, a bypass circuit 6 that bypasses the corresponding detection current Is during recording and an attenuation circuit that drives this are provided. A container 10 is provided.
側路回路6はトランジスタ61と抵抗62およびトラン
ジスタ63と抵抗64とを図示のように組み合わせた構
成になっている。The bypass circuit 6 has a configuration in which a transistor 61 and a resistor 62 and a transistor 63 and a resistor 64 are combined as shown.
側路回路6は一方のトランジスタ61に電流1oを流入
させた場合に他方のトランジスタ63に電流1゜と同値
の電流Is = Ioを流入させることができるので定
電流回路の構成によ(用いられることで知られている。When the current 1o flows into one transistor 61, the bypass circuit 6 can allow a current Is = Io of the same value as the current 1° to flow into the other transistor 63. Therefore, depending on the configuration of the constant current circuit (used It is known for that.
第5図は従来例の電流対光出力特性曲線であって、半導
体レーザと光量検知器の特性を示す。第4図と第5図に
おいて、半導体レーザ1に再生時の駆動電流1bを流し
た時の光出力をPrとし、光出力Prに対応する光量検
知器3の全検出電流Ipdすなわちこの場合は検出電流
Irだけを電圧変換してAPC回路21にフィードバッ
クし、APC回路21は半導体レーザ1の再生時におけ
る光出力Prが一定値になるように駆動電流rbを制御
する。FIG. 5 is a current vs. light output characteristic curve of a conventional example, showing the characteristics of a semiconductor laser and a light amount detector. 4 and 5, the optical output when the drive current 1b is applied to the semiconductor laser 1 during reproduction is Pr, and the total detection current Ipd of the light amount detector 3 corresponding to the optical output Pr, that is, in this case, the detection Only the current Ir is converted into a voltage and fed back to the APC circuit 21, and the APC circuit 21 controls the drive current rb so that the optical output Pr during reproduction of the semiconductor laser 1 becomes a constant value.
また、半導体レーザlに記録電流■−を重畳して流した
ときの全光出力をPwとし、記録電流顔に対応する光量
検知器3の重畳検出電流をIsとすると、光量検知器3
の全検出電流1pd = Ir + Isとなり、この
全検出電流Ipdを抵抗4で電圧変換すると重畳検出電
流Isの成分だけが余分となって再生電流rbが変化し
てしまう。Further, if the total optical output when a recording current ■- is superimposed and passed through the semiconductor laser l is Pw, and the superimposed detection current of the light amount detector 3 corresponding to the recording current face is Is, then the light amount detector 3
The total detection current 1pd = Ir + Is, and when this total detection current Ipd is converted into voltage by the resistor 4, only the component of the superimposed detection current Is becomes redundant, and the reproduction current rb changes.
そこで重畳検出電流Isだけを側路回路6のトランジス
タ13に流入させるようにトランジスタ1)にながれる
電流Ioを制御すればよいことが分かる。Therefore, it can be seen that the current Io flowing through the transistor 1) should be controlled so that only the superimposition detection current Is flows into the transistor 13 of the bypass circuit 6.
ところでこの重畳検出電流Isは第2図から分かるよう
に記録電流1wに比例する。その係数を1/にとすれば
減衰器10を用いてその出力電流IoをIw/kに設定
することは容易である。By the way, as can be seen from FIG. 2, this superimposition detection current Is is proportional to the recording current 1w. If the coefficient is set to 1/, it is easy to set the output current Io to Iw/k using the attenuator 10.
従って重畳検出電流Is = Io = Iw/ kと
なるように減衰器10の係数1/kを設定することによ
り、抵抗4には再生電流Ibに対応する検出電流Irの
みが流れることになり矛盾は解決される。Therefore, by setting the coefficient 1/k of the attenuator 10 so that the superimposed detection current Is = Io = Iw/k, only the detection current Ir corresponding to the reproduction current Ib flows through the resistor 4, and the contradiction is resolved. resolved.
一般に半導体レーザの電流対光出力特性は第5図に示す
ように一つの折点を有する折線形であり、半導体レーザ
の光出力に対応する光量検知器の出力電流特性は直線形
である。Generally, the current vs. light output characteristic of a semiconductor laser is a folded line having one breakpoint as shown in FIG. 5, and the output current characteristic of a light amount detector corresponding to the light output of the semiconductor laser is a linear shape.
従って記録電流I−に比例して光量検知器3に流れる検
出電流Isの電流比は折点Pを境にして異なる値を示す
。記録電流1wの変化範囲が折点Pより増加方向の領域
にあるときは一つの比例係数を設定するだけでよいが、
折点Pより減少方向の領域を含むようになると、一つの
減衰器10だけでは側路回路6に分岐させるべき電流値
に誤差が発生し、変調波形が乱れる欠点がある。Therefore, the current ratio of the detection current Is flowing through the light amount detector 3 in proportion to the recording current I- exhibits different values with the corner point P as a boundary. When the range of change of the recording current 1w is in the increasing direction from the breaking point P, it is only necessary to set one proportionality coefficient.
When a region in the decreasing direction is included from the corner point P, using only one attenuator 10 has the disadvantage that an error occurs in the current value to be branched to the bypass circuit 6, and the modulation waveform is disturbed.
本発明は上記従来の欠点に鑑み創作されたもので、分岐
電流に誤差の発生しない回路の提供を目的とする。The present invention was created in view of the above-mentioned drawbacks of the conventional art, and an object of the present invention is to provide a circuit in which errors do not occur in branch currents.
第1図は本発明の原理説明図を示す。図において、1は
半導体レーザ、2は半導体レーザに所定の再生電流また
は該再生電流に重畳して記録電流を供給する駆動回路で
ある。3は半導体レーザの出射光量をモニタする光量検
知器、4は抵抗、5はループ回路であって、前記再生電
流に対応する光量検知器3の出力電流1rを抵抗4にて
電圧変換して駆動回路2にフィードバックする回路であ
る。FIG. 1 shows a diagram explaining the principle of the present invention. In the figure, 1 is a semiconductor laser, and 2 is a drive circuit that supplies a predetermined reproduction current or a recording current superimposed on the reproduction current to the semiconductor laser. 3 is a light amount detector for monitoring the amount of light emitted from the semiconductor laser, 4 is a resistor, and 5 is a loop circuit, which is driven by converting the output current 1r of the light amount detector 3 corresponding to the reproduction current into a voltage using the resistor 4. This is a circuit that feeds back to circuit 2.
6は側路回路であって前記記録電流に対応する光量検知
器3の出力電流Isを光量検知器3の全出力電流Ipd
=Ir+Isから分岐する機能を持つ回路である。6 is a bypass circuit which converts the output current Is of the light amount detector 3 corresponding to the recording current to the total output current Ipd of the light amount detector 3.
=Ir+Is This is a circuit that has a function of branching from Is.
このように構成された半導体レーザ駆動回路において、
前記全出力電流Tpdを電圧変換する抵抗7と該抵抗7
の出力電圧を所要の閾値Ewと比較する比較回路8を設
け、該比較回路8の出力にて前記側路回路6の分岐電流
を切換え制御する手段9、すなわち低電流減衰器81と
高電流減衰器82およびこれらを切換え制御するマルチ
プレクサ83とを設けたことを特徴とする光学的記録再
生装置を提供することにより本発明の目的は達成される
。In the semiconductor laser drive circuit configured in this way,
a resistor 7 that converts the total output current Tpd into voltage; and the resistor 7
A comparison circuit 8 is provided for comparing the output voltage of the output voltage with a required threshold value Ew, and means 9 for switching and controlling the branch current of the bypass circuit 6 using the output of the comparison circuit 8, that is, a low current attenuator 81 and a high current attenuation The object of the present invention can be achieved by providing an optical recording/reproducing apparatus characterized in that it is equipped with a multiplexer 82 and a multiplexer 83 for switching and controlling these.
半導体レーザ1の電流対先出力特性における折点位置に
対応する光量検知器3の出力電流が、抵抗7にて変換さ
れる電圧を閾値E−に設定し、比較回路8の入力が閾値
Ew以下の場合には低電流減衰器91を選択し、閾値E
−以上の場合には高電流減衰器92を選択するようにマ
ルチプレクサ93を切換え制御することにより、半導体
レーザの低光出力領域においても誤差なく再生時と記録
時の駆動電流を区別して供給することができる。The voltage at which the output current of the light amount detector 3 corresponding to the corner position in the current vs. output characteristic of the semiconductor laser 1 is converted by the resistor 7 is set to a threshold value E-, and the input of the comparator circuit 8 is below the threshold value Ew. In this case, select the low current attenuator 91 and set the threshold E
- In the above case, by switching and controlling the multiplexer 93 to select the high current attenuator 92, it is possible to separately supply drive currents for reproduction and recording without error even in the low optical output region of the semiconductor laser. I can do it.
以下本発明の実施例を図面によって詳述する。 Embodiments of the present invention will be described in detail below with reference to the drawings.
なお、構成、動作の説明を理解し易くするために各図を
通じて同一部分には同一符号を付してその重複説明を省
略する。In order to make the explanation of the configuration and operation easier to understand, the same parts are denoted by the same reference numerals throughout the drawings, and repeated explanation thereof will be omitted.
第2図は本発明の詳細な説明図を示す。図において、7
は光量検知器3の全出力電流1pdを電圧に変換するた
めの手段として用いられる抵抗である。FIG. 2 shows a detailed illustration of the invention. In the figure, 7
is a resistor used as a means for converting the total output current 1 pd of the light amount detector 3 into a voltage.
8は比較回路であって、その入力端子の一方には所要の
閾値Ewが常時印加され、他方の入力端子には抵抗7に
流れる電流1pdによってできた変換電圧が入力される
。Reference numeral 8 denotes a comparator circuit, to which a required threshold value Ew is always applied to one of its input terminals, and a converted voltage generated by the current 1 pd flowing through the resistor 7 is input to the other input terminal.
9は側路回路6の分岐電流を切換え制御する手段であっ
て、例えば分岐電流を規制する手段として低電流減衰器
91と高電流減衰器92を設け、切換え手段としてマル
チプレクサ93を用いた構成になっている。マルチプレ
クサ93は比較回路8の出力にて制御される。Reference numeral 9 denotes means for switching and controlling the branch current of the bypass circuit 6, and for example, a low current attenuator 91 and a high current attenuator 92 are provided as means for regulating the branch current, and a multiplexer 93 is used as the switching means. It has become. Multiplexer 93 is controlled by the output of comparison circuit 8.
第3図は本発明の電流対先出力特性曲線であって、半導
体レーザ1と光量検知器3の動作電流を説明する特性曲
線である。図において、半導体レーザ■の特性は折点P
を有する折線形であり、光量検知器3の特性は直線形で
ある。ここでは記録電流夏−の動作範囲が折点Pを含む
場合について考える。FIG. 3 is a current versus output characteristic curve of the present invention, which is a characteristic curve illustrating the operating current of the semiconductor laser 1 and the light amount detector 3. In the figure, the characteristics of the semiconductor laser ■ are at the bending point P
The characteristic of the light amount detector 3 is a linear shape. Here, a case will be considered in which the operating range of the recording current includes the breaking point P.
すなわち、記録電流Iwに比例して流れる光量検知器3
の出力電流Isの電流比Is/I−は折点前の領域Aで
は1/にい折点後の領域Bでは17に2の二つに分けら
れる。That is, the light quantity detector 3 flows in proportion to the recording current Iw.
The current ratio Is/I- of the output current Is is divided into two parts: 1/I- in the region A before the break point and 1/2 in the region B after the break point.
第2図と第3図において、折点Pに対応する光量検知器
3の出力電流をIOとし、第2図における光量検知器3
の全出力電流1pd = ioとなったときに、抵抗7
の発生する変換電圧が閾値E−となるように比較回路8
の入力に常時印加する。In FIGS. 2 and 3, the output current of the light amount detector 3 corresponding to the breaking point P is set as IO, and the light amount detector 3 in FIG.
When the total output current of 1 pd = io, the resistor 7
The comparator circuit 8
Always applied to the input.
従って、抵抗7の変換電圧が閾値Ew以下のときの比較
回路8の出力を“0″とすれば、この信号″0”にてマ
ルチプレクサ93をトリガし、低電流減衰器91に接続
されるように切換える。低電流減衰器91は変調回路2
2の出力をIw/に、に変換するように設定された減衰
器である。Therefore, if the output of the comparator circuit 8 is set to "0" when the converted voltage of the resistor 7 is less than the threshold value Ew, the multiplexer 93 is triggered by this signal "0" and connected to the low current attenuator 91. Switch to The low current attenuator 91 is the modulation circuit 2
This is an attenuator configured to convert the output of 2 to Iw/.
同様にして抵抗7の変換電圧が閾値Ew以上のときは、
比較回路8の出力は“1”となってマルチプレクサ93
をトリガし、高電流減衰器92に接続されるように切換
えられる。高電流減衰器92は変調回路22の出力をI
w/kzに変換するように設定された減衰器である。Similarly, when the converted voltage of the resistor 7 is equal to or higher than the threshold value Ew,
The output of the comparator circuit 8 becomes “1” and is sent to the multiplexer 93.
, and is switched to be connected to high current attenuator 92. A high current attenuator 92 reduces the output of the modulation circuit 22 to I
The attenuator is set to convert to w/kz.
以上詳細に説明したように本発明の光学的記録再生装置
によれば、常に再生時の半導体レーザの光出力を一定に
すると共に、全ての光出力領域にわたり所望の記録用の
光出力を得ることができる。As explained in detail above, according to the optical recording/reproducing apparatus of the present invention, it is possible to always keep the optical output of the semiconductor laser constant during reproduction and to obtain the desired optical output for recording over the entire optical output range. I can do it.
第1図は本発明の原理説明図、
第2図は本発明の詳細な説明図、
第3図は本発明の電流対光出力特性曲線、第4図は従来
の半導体レーザ駆動回路のブロック図、
第5図は従来例の電流対光出力特性曲線を示す。
図において、1は半導体レーザ、2は駆動回路、3は光
量検知器、4と7は抵抗、5はループ回路、6は側路回
路、8は比較回路、9は分岐電流を切換え制御する手段
をそれぞれ示す。
第3図
男
名し求の千黒停し−γ耳1重〃圓鍔蛸プロ17図第4F
!!JFig. 1 is an explanatory diagram of the principle of the present invention, Fig. 2 is a detailed explanatory diagram of the present invention, Fig. 3 is a current vs. optical output characteristic curve of the present invention, and Fig. 4 is a block diagram of a conventional semiconductor laser drive circuit. , FIG. 5 shows a current versus light output characteristic curve of a conventional example. In the figure, 1 is a semiconductor laser, 2 is a drive circuit, 3 is a light amount detector, 4 and 7 are resistors, 5 is a loop circuit, 6 is a bypass circuit, 8 is a comparison circuit, and 9 is a means for switching and controlling the branch current. are shown respectively. Figure 3 Senkuro stop of a man's name - γ ear 1 layer Entsuba Tako Pro 17 Figure 4F
! ! J
Claims (1)
に重畳して記録電流を供給する駆動回路(2)と、前記
半導体レーザ(1)の出射光量をモニタする光量検知器
(3)と、 前記再生電流に対応する前記光量検知器(3)の出力電
流(Ir)を、抵抗(4)にて電圧変換して前記駆動回
路(2)に負帰還するループ回路(5)と、前記記録電
流に対応する前記光量検知器(3)の出力電流(Is)
を前記光量検知器(3)の全出力電流(Ipd)から分
岐する側路回路(6)とから構成されてなる半導体レー
ザ駆動回路において、 前記全出力電流(Ipd)を電圧変換する抵抗(7)と
、該抵抗(7)の出力電圧を所要の閾値(Ew)と比較
する比較回路(8)とを付設し、 該比較回路(8)の出力にて前記側路回路(6)の分岐
電流を切り換え制御する手段(9)を設けたことを特徴
とする光学的記録再生装置。[Scope of Claims] A drive circuit (2) that supplies a predetermined reproduction current or a recording current superimposed on the reproduction current to the semiconductor laser (1), and a light amount detector that monitors the amount of light emitted from the semiconductor laser (1). a loop circuit (3) that converts the output current (Ir) of the light amount detector (3) corresponding to the reproduction current into a voltage with a resistor (4) and negatively feeds it back to the drive circuit (2); 5) and an output current (Is) of the light amount detector (3) corresponding to the recording current.
and a bypass circuit (6) that branches from the total output current (Ipd) of the light amount detector (3), a resistor (7) that converts the total output current (Ipd) into a voltage. ) and a comparison circuit (8) that compares the output voltage of the resistor (7) with a required threshold (Ew), and the branch of the bypass circuit (6) is provided at the output of the comparison circuit (8). An optical recording/reproducing device characterized in that it is provided with means (9) for switching and controlling current.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP60034941A JPS61194649A (en) | 1985-02-22 | 1985-02-22 | Optical recording and reproducing device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP60034941A JPS61194649A (en) | 1985-02-22 | 1985-02-22 | Optical recording and reproducing device |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS61194649A true JPS61194649A (en) | 1986-08-29 |
Family
ID=12428200
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP60034941A Pending JPS61194649A (en) | 1985-02-22 | 1985-02-22 | Optical recording and reproducing device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS61194649A (en) |
-
1985
- 1985-02-22 JP JP60034941A patent/JPS61194649A/en active Pending
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