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JPH0626266B2 - Light emitting element drive - Google Patents
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JPH0626266B2 - Light emitting element drive - Google Patents

Light emitting element drive

Info

Publication number
JPH0626266B2
JPH0626266B2 JP19411684A JP19411684A JPH0626266B2 JP H0626266 B2 JPH0626266 B2 JP H0626266B2 JP 19411684 A JP19411684 A JP 19411684A JP 19411684 A JP19411684 A JP 19411684A JP H0626266 B2 JPH0626266 B2 JP H0626266B2
Authority
JP
Japan
Prior art keywords
light emitting
emitting element
circuit
input
signal
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
JP19411684A
Other languages
Japanese (ja)
Other versions
JPS6171687A (en
Inventor
一郎 山下
敏之 土屋
岳司 木下
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.)
NTT Inc
Original Assignee
Nippon Telegraph and Telephone Corp
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 Nippon Telegraph and Telephone Corp filed Critical Nippon Telegraph and Telephone Corp
Priority to JP19411684A priority Critical patent/JPH0626266B2/en
Publication of JPS6171687A publication Critical patent/JPS6171687A/en
Publication of JPH0626266B2 publication Critical patent/JPH0626266B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S5/00Semiconductor lasers
    • H01S5/06Arrangements for controlling the laser output parameters, e.g. by operating on the active medium
    • H01S5/068Stabilisation of laser output parameters
    • H01S5/06808Stabilisation of laser output parameters by monitoring the electrical laser parameters, e.g. voltage or current

Landscapes

  • Physics & Mathematics (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • General Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Optics & Photonics (AREA)
  • Semiconductor Lasers (AREA)
  • Led Devices (AREA)
  • Optical Communication System (AREA)

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、光通信装置に利用される。たとえば、ベース
バンドのテレビジョン信号を光振幅変調して光フアイバ
に伝送する装置に利用される。とくに、発光出力強度を
入力信号により振幅変調する装置の駆動装置に関する。
DETAILED DESCRIPTION OF THE INVENTION [Industrial field of application] The present invention is applied to an optical communication device. For example, it is used in an apparatus for optical-amplitude-modulating a baseband television signal and transmitting it to an optical fiber. In particular, the present invention relates to a driving device of a device that amplitude-modulates a light emission output intensity by an input signal.

〔従来の技術〕[Conventional technology]

発光素子の出力光強度は一般に駆動電流の大きさに対し
て非直線であり、駆動電流が大きくなるとその出力強度
は比例して大きくならない。従来、これを補償するため
に、第5図に示すような駆動回路が用いられている。こ
の回路は入力端子Siに入力される信号をトランジスタ
Qにより増幅して出力端子Soに送出し、発光素子ED
を駆動する回路であり、エミッタ回路に複数i個のダイ
オードを並列に接続して、発光素子の非直線性を逆に補
償するように構成されている。すなわち、入力端子Si
の信号レベルがきわめて低いときには、すべてのダイオ
ードD〜Diが導通状態にあり、トランジスタQの利
得は小さく制限されているが、入力端子Siの信号レベ
ルが高くなると、それに応じてダイオードが順に非導通
状態になって、トランジスタQの利得が次第に大きくな
るように構成されている。
The output light intensity of the light emitting element is generally non-linear with respect to the magnitude of the drive current, and the output intensity does not increase proportionally as the drive current increases. Conventionally, in order to compensate for this, a drive circuit as shown in FIG. 5 has been used. This circuit amplifies the signal input to the input terminal Si by the transistor Q and sends the amplified signal to the output terminal So, so that the light emitting element ED
Is a circuit that drives a plurality of i diodes in parallel to the emitter circuit, and is configured to reversely compensate the nonlinearity of the light emitting element. That is, the input terminal Si
When the signal level of is extremely low, all the diodes D 1 to Di are in the conductive state, and the gain of the transistor Q is limited to a small value. However, when the signal level of the input terminal Si becomes high, the diodes are sequentially turned off. It is configured such that the transistor Q becomes conductive and the gain of the transistor Q gradually increases.

この回路は、ある程度までその非直線性を補償すること
ができるが、発光素子EDの特性に対して個別に調整を
行うことが必要であり、製造工数が大きい。また、閉ル
ープの制御ではないので、安定性に欠ける欠点がある。
This circuit can compensate for the non-linearity to some extent, but it is necessary to individually adjust the characteristics of the light emitting element ED, and the number of manufacturing steps is large. Further, since it is not a closed loop control, there is a drawback that the stability is lacking.

第6図は従来例の別の構成図である。この例は入力端子
Siの信号が駆動回路DRで増幅されて出力端子Soに
現れ、発光素子EDを発光させる。この発光の一部を受
光素子PDで受光してその信号を増幅器AMPで増幅
し、駆動回路DRの入力に負帰還接続するものである。
この回路は全体が閉ループの制御回路になっているの
で、その動作は安定であり、素子の特性ばらつきを相当
程度に吸収するが、受光素子PDを必要とすること、こ
のために光信号を分岐する光回路を必要とすること、こ
の光回路の機構が電気回路にくらべて不安定であること
などの欠点がある。
FIG. 6 is another block diagram of the conventional example. In this example, the signal at the input terminal Si is amplified by the drive circuit DR and appears at the output terminal So, causing the light emitting element ED to emit light. A part of this light emission is received by the light receiving element PD, its signal is amplified by the amplifier AMP, and negative feedback connection is made to the input of the drive circuit DR.
Since this circuit is a closed loop control circuit as a whole, its operation is stable and absorbs the characteristic variations of the elements to a considerable extent, but it requires the light receiving element PD, and therefore the optical signal is branched. There are drawbacks such as the need for an optical circuit to operate and the mechanism of this optical circuit being more unstable than an electric circuit.

〔発明が解決しようとする問題点〕[Problems to be solved by the invention]

本発明はこれを改良するもので、動作が安定であり、機
構が簡単な発光素子の非直線性を補償することができる
駆動装置を提供することを目的とする。
An object of the present invention is to improve the above and to provide a driving device which is stable in operation and which can compensate the non-linearity of a light emitting element having a simple mechanism.

〔問題点を解決するための手段〕[Means for solving problems]

本発明は、入力端子の信号を増幅し出力端子に送出し、
この出力端子に接続される発光素子をほぼ一定の電源イ
ンピーダンスで駆動する駆動回路を備えた発光素子駆動
装置において、 上記出力端子の電圧を入力とする入力インピーダンスの
高い電圧検出回路と、この電圧検出回路の出力を上記駆
動回路の入力に負帰還結合する回路とを備えたことを特
徴とする。
The present invention amplifies the signal at the input terminal and sends it to the output terminal,
In a light emitting element drive device equipped with a drive circuit for driving a light emitting element connected to this output terminal with a substantially constant power source impedance, a voltage detection circuit with a high input impedance that inputs the voltage of the output terminal, and this voltage detection circuit And a circuit for negatively feedback coupling the output of the circuit to the input of the drive circuit.

〔作用〕[Action]

発光素子に半導体を用いると、その電流と発光強度との
関係が非直線になる領域では、その発光素子自体のイン
ピーダンスが非直線になり、この影響が端子電圧に現れ
る。これは、半導体素子の端子電圧の変化量が半導体の
活性層内のキャリア密度と密接な関係があるためと考え
られる。したがって、ほぼ一定の電源インピーダンスの
駆動回路で発光素子を駆動するとき、その端子電圧を負
帰還結合することにより、発光特性の非直線特性を相当
程度に改善することができる。
When a semiconductor is used for the light emitting element, the impedance of the light emitting element itself becomes non-linear in a region where the relation between the current and the light emission intensity becomes non-linear, and this effect appears in the terminal voltage. It is considered that this is because the amount of change in the terminal voltage of the semiconductor element is closely related to the carrier density in the active layer of the semiconductor. Therefore, when the light emitting element is driven by the driving circuit having a substantially constant power source impedance, the non-linear characteristic of the light emitting characteristic can be considerably improved by negatively feedback coupling the terminal voltage.

〔実施例〕〔Example〕

第1図は本発明実施例装置の基本的なブロック構成図で
ある。入力端子Siに与えらえる信号(一例としてベー
スバンドのテレビジョン信号)は駆動回路DRにより増
幅されて出力端子Soに現れる。この出力端子nは半導
体レーザによる発光素子EDが接続される。ここで、本
発明の特徴とするところは、この出力端子Soに電圧検
出回路DETが接続され、その出力が駆動回路DRの入
力に負帰還結合されたところにある。この電圧検出回路
DETはその入力インピーダンスが、駆動回路DRの出
力インピーダンスおよび発光素子EDのインピーダンス
より十分に高く設定されていて、発光素子EDの端子電
圧をその動作に影響を与えずに検出できるように構成さ
れている。
FIG. 1 is a basic block diagram of the apparatus of the present invention. A signal given to the input terminal Si (a baseband television signal as an example) is amplified by the drive circuit DR and appears at the output terminal So. The output terminal n is connected to the light emitting element ED of a semiconductor laser. Here, the feature of the present invention resides in that the voltage detection circuit DET is connected to the output terminal So and the output thereof is negatively feedback-coupled to the input of the drive circuit DR. The input impedance of the voltage detection circuit DET is set sufficiently higher than the output impedance of the drive circuit DR and the impedance of the light emitting element ED so that the terminal voltage of the light emitting element ED can be detected without affecting its operation. Is configured.

この回路では、発光素子EDの発光特性にしたがって変
動する端子電圧が、駆動回路DRの入力に負帰還されて
線形の駆動を実現する。
In this circuit, the terminal voltage that varies according to the light emission characteristics of the light emitting element ED is negatively fed back to the input of the drive circuit DR to realize linear driving.

第2図はこの実施例回路の具体的な回路図である。図中
の破線により駆動回路DR、電圧検出回路DETおよび
発光素子EDを示す。すなわち、入力端子Siの信号は
2個のトランジスタQおよびQにより増幅され、ト
ランジスタQのコレクタに接続された出力端子Soか
らの、発光素子EDに供給される。この出力端子Soの
電圧はコンデンサCoにより、電界効果トランジスタQ
のゲートに供給され、この電界効果トランジスタQ
のドレイン出力は入力端子Siに帰還接続される。
FIG. 2 is a concrete circuit diagram of this embodiment circuit. The drive circuit DR, the voltage detection circuit DET, and the light emitting element ED are indicated by broken lines in the figure. That is, the signal of the input terminal Si is amplified by the two transistors Q 1 and Q 2 and supplied to the light emitting element ED from the output terminal So connected to the collector of the transistor Q 2 . The voltage at the output terminal So is applied to the field effect transistor Q by the capacitor Co.
3 is supplied to the gate of the field effect transistor Q 3
The drain output of is feedback-connected to the input terminal Si.

この構成では駆動装置全体が負帰還ループを形成して直
接性のよい安定な駆動を行うことができる。
With this configuration, the entire driving device can form a negative feedback loop to perform stable driving with good directness.

第3図および第4図はこの実施例装置の試験結果を示す
図である。第3図は、第2図に示すコンデンサCoの接
続を切り離して、この装置の負帰還ループを切断した状
態(開ループの状態)で発光素子EDを駆動し、この発
光素子EDの光出力信号を受光素子で受光してその周波
数成分をスペクトルアナライザで分析した結果の信号波
形図を示す。第4図は、コンデンサCoを接続して第2
図に示す本発明実施例の状態(開ループ状態)で発光素
子EDを駆動し、その光出力信号の周波数成分をスペク
トルアナライザで分析した結果の信号波形図を示す。
3 and 4 are diagrams showing the test results of the apparatus of this embodiment. FIG. 3 shows that the light emitting element ED is driven in a state (open loop state) in which the negative feedback loop of this device is disconnected by disconnecting the connection of the capacitor Co shown in FIG. FIG. 6 is a signal waveform diagram of a result of receiving light from a light receiving element and analyzing the frequency component with a spectrum analyzer. FIG. 4 shows the second circuit with the capacitor Co connected.
The signal waveform diagram of the result of having driven the light emitting element ED in the state of the Example of this invention shown in the figure (open loop state), and having analyzed the frequency component of the optical output signal with the spectrum analyzer is shown.

入力端子Siの信号は600kHzの正弦波である。第3図お
よび第4図の横軸は周波数(リニア)、縦軸は振幅(相
対値、dB)である。第3図、第4図においてfoは入力
信号と同じ600kHz、2foは入力信号の2次高調波の12
00kHzを、3foは3次高調波の1800kHzを示す。
The signal at the input terminal Si is a 600 kHz sine wave. 3 and 4, the horizontal axis represents frequency (linear) and the vertical axis represents amplitude (relative value, dB). In FIGS. 3 and 4, fo is the same as the input signal, 600 kHz, and 2fo is the second harmonic of the input signal, 12
00kHz and 3fo indicate the third harmonic 1800kHz.

この図からわかるように、負帰還ループを用いずに開ル
ープの状態で駆動したときには、第二および第三高調波
が観測されるが、負帰還ループを用いることにより直線
性が向上し、高調波が観測できなくなることがわかる。
As can be seen from this figure, the second and third harmonics are observed when driven in the open loop state without using the negative feedback loop, but using the negative feedback loop improves linearity and You can see that the waves can no longer be observed.

この実施例回路では、負帰還回路の総合ループ利得(μ
β)は約16dBであり、閉ループの状態と開ループの状態
との発光歪改善量は約14dBであった。すなわち、本発明
の装置では発光素子EDは負帰還ループの外にあり、発
光素子自体の非直線性はこの負帰還ループにより改善さ
れないが、この試験により発光歪のうち大部分は駆動回
路の側に有効な負帰還を施すことにより改善されること
がわかった。
In this example circuit, the total loop gain (μ
β) was about 16 dB, and the amount of emission distortion improvement in the closed loop state and the open loop state was about 14 dB. That is, in the device of the present invention, the light emitting element ED is outside the negative feedback loop, and although the non-linearity of the light emitting element itself is not improved by this negative feedback loop, this test shows that most of the light emission distortion is on the drive circuit side. It has been found that this can be improved by applying effective negative feedback to.

〔発明の効果〕〔The invention's effect〕

以上説明したように、本発明によれば、負帰還ループに
より素子のばらつきを吸収するので個別の調整が不要で
ある。負帰還ループを用いるのでその動作が安定であ
る。また光回路がループ内に含まれないので構成が簡単
である。本発明はアナログのテレビジョン信号を光フア
イバに伝送する方式に利用してきわめて有効である。
As described above, according to the present invention, since the negative feedback loop absorbs the variation of the elements, individual adjustment is not necessary. Since the negative feedback loop is used, its operation is stable. Moreover, since the optical circuit is not included in the loop, the configuration is simple. The present invention is extremely effective when applied to a system for transmitting an analog television signal to an optical fiber.

【図面の簡単な説明】 第1図は本発明実施例装置のブロック構成図。 第2図は本発明実施例装置の具体的な回路図。 第3図および第4図は本発明実施例装置の試験結果を示
す信号のオシロ波形図。 第5図および第6図は従来例装置の構成図。
BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a block diagram of an apparatus according to an embodiment of the present invention. FIG. 2 is a concrete circuit diagram of the device of the present invention. FIG. 3 and FIG. 4 are oscillographic waveform diagrams of signals showing the test results of the apparatus of the present invention. 5 and 6 are configuration diagrams of a conventional example device.

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】入力端子の信号を増幅し出力端子に送出
し、この出力端子に接続される発光素子をほぼ一定の電
源インピーダンスで駆動する駆動回路を備えた発光素子
駆動装置において、 上記出力端子の電圧を入力とする入力インピーダンスの
高い電圧検出回路と、 この電圧検出回路の出力を上記駆動回路の入力に負帰還
結合する回路と を備えたことを特徴とする発光素子駆動装置。
1. A light emitting element drive device comprising a drive circuit for amplifying a signal from an input terminal, sending the amplified signal to an output terminal, and driving a light emitting element connected to the output terminal with a substantially constant power source impedance. 2. A light emitting element drive device comprising: a voltage detection circuit having a high input impedance, which receives the voltage of FIG. 3 as an input, and a circuit for negatively feedback coupling the output of the voltage detection circuit to the input of the drive circuit.
【請求項2】発光素子が半導体レーザである特許請求の
範囲第(1)項に記載の発光素子駆動装置。
2. The light emitting element drive device according to claim 1, wherein the light emitting element is a semiconductor laser.
JP19411684A 1984-09-14 1984-09-14 Light emitting element drive Expired - Lifetime JPH0626266B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP19411684A JPH0626266B2 (en) 1984-09-14 1984-09-14 Light emitting element drive

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP19411684A JPH0626266B2 (en) 1984-09-14 1984-09-14 Light emitting element drive

Publications (2)

Publication Number Publication Date
JPS6171687A JPS6171687A (en) 1986-04-12
JPH0626266B2 true JPH0626266B2 (en) 1994-04-06

Family

ID=16319183

Family Applications (1)

Application Number Title Priority Date Filing Date
JP19411684A Expired - Lifetime JPH0626266B2 (en) 1984-09-14 1984-09-14 Light emitting element drive

Country Status (1)

Country Link
JP (1) JPH0626266B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP5097628B2 (en) * 2008-07-03 2012-12-12 パナソニック株式会社 Semiconductor light source driving apparatus and semiconductor light source driving method

Also Published As

Publication number Publication date
JPS6171687A (en) 1986-04-12

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