JP2684697B2 - Semiconductor laser drive circuit - Google Patents

Semiconductor laser drive circuit

Info

Publication number
JP2684697B2
JP2684697B2 JP20591688A JP20591688A JP2684697B2 JP 2684697 B2 JP2684697 B2 JP 2684697B2 JP 20591688 A JP20591688 A JP 20591688A JP 20591688 A JP20591688 A JP 20591688A JP 2684697 B2 JP2684697 B2 JP 2684697B2
Authority
JP
Japan
Prior art keywords
resistor
semiconductor laser
effect transistor
drive circuit
field
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
JP20591688A
Other languages
Japanese (ja)
Other versions
JPH0254977A (en
Inventor
千隆 小西
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.)
NEC Corp
Original Assignee
NEC 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 NEC Corp filed Critical NEC Corp
Priority to JP20591688A priority Critical patent/JP2684697B2/en
Publication of JPH0254977A publication Critical patent/JPH0254977A/en
Application granted granted Critical
Publication of JP2684697B2 publication Critical patent/JP2684697B2/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
    • H01S5/04Processes or apparatus for excitation, e.g. pumping, e.g. by electron beams
    • H01S5/042Electrical excitation ; Circuits therefor

Landscapes

  • Physics & Mathematics (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • General Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Optics & Photonics (AREA)
  • Semiconductor Lasers (AREA)

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は、半導体レーザの駆動回路に関し、特に、GH
zを超える高速デイジタル光通信の送信部等に用いられ
る電界効果形トランジスタを用いた、半導体レーザを駆
動する回路に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a semiconductor laser drive circuit, and more particularly to a GH
The present invention relates to a circuit for driving a semiconductor laser, which uses a field-effect transistor used in a transmitting section of high-speed digital optical communication exceeding z.

(従来の技術) 第2図に従来の半導体レーザ駆動回路の一例を示す。(Prior Art) FIG. 2 shows an example of a conventional semiconductor laser drive circuit.

従来この種の半導体レーザの駆動回路は電界効果形ト
ランジスタ1のソース電極Sと基準電位9間にコンデン
サ3を接続し、ソース電極Sと電源V間に抵抗2を接続
し、電界効果形トランジスタ1のドレイン電極Dと基準
電位間に、抵抗4と半導体レーザ5の直列回路を接続
し、抵抗4にコンデンサ8を並列接続し、さらに半導体
レーザ5のカソードに直流バイアス供給回路6を接続し
た構成となつている。
In the conventional driving circuit of this type of semiconductor laser, the capacitor 3 is connected between the source electrode S of the field effect transistor 1 and the reference potential 9, and the resistor 2 is connected between the source electrode S and the power source V. Between the drain electrode D and the reference potential, a resistor 4 and a semiconductor laser 5 are connected in series, a resistor 8 is connected in parallel with a capacitor 8, and a direct current bias supply circuit 6 is connected to the cathode of the semiconductor laser 5. I'm running.

(発明が解決しようとする課題) この従来の半導体レーザ駆動回路は、半導体レーザ5
の発振遅延等によるパターン効果を補償するために抵抗
4にスピードアツプコンデンサ8が並列接続されている
が、周波数が高くなるにつれ、実装の影響や半導体レー
ザのバラツキが大きくなるので、光波形補償用コンデン
サ8の値も変えて最良の光波形とする必要がある。しか
しながら、従来の回路は第2図のような構成であるの
で、コンデンサ8を取り替えて光波形のパターン効果を
補償しなければならず、補償容量の連続的可変が不可能
であるという欠点がある。
(Problems to be Solved by the Invention) This conventional semiconductor laser drive circuit is provided with a semiconductor laser 5
A speed-up capacitor 8 is connected in parallel with the resistor 4 in order to compensate for the pattern effect due to the oscillation delay, etc. However, as the frequency becomes higher, the influence of mounting and the variation of the semiconductor laser become larger. It is necessary to change the value of the condenser 8 to obtain the best optical waveform. However, since the conventional circuit has the configuration as shown in FIG. 2, it is necessary to replace the capacitor 8 to compensate for the pattern effect of the optical waveform, and there is a drawback that the compensation capacitance cannot be continuously varied. .

本発明の目的は上記欠点を解決するもので、電界効果
形トランジスタのドレインとレーザダイオードの間の抵
抗端子間の容量を連続的に変えることができる半導体レ
ーザ駆動回路を提供することにある。
An object of the present invention is to solve the above drawbacks and to provide a semiconductor laser drive circuit capable of continuously changing the capacitance between the resistance terminals between the drain of the field effect transistor and the laser diode.

(課題を解決するための手段) 前記目手を達成するために本発明による半導体レーザ
駆動回路は電界効果トランジスタのソース電極と基準電
位との間に第1のコンデンサを接続し、前記ソース電極
と電源との間に第1の抵抗を接続し、前記電界効果トラ
ンジスタのドレイン電極と基準電位との間に、第2の抵
抗とレーザダイオードの直列回路を接続し、前記第2の
抵抗とレーザダイオードの共通接続点に直流バイアス供
給回路を接続し、さらに前記第2の抵抗と並列に第2の
コンデンサを接続してなり、前記電界効果形トランジス
タのゲートにパルス電流を供給することにより前記レー
ザダイオードを発振させる半導体レーザ駆動回路におい
て、前記第2のコンデンサの代わりに前記第2の抵抗に
並列に第2の電界効果形トランジスタを接続し、前記第
2の電界効果形トランジスタのゲート電圧を制御するこ
とにより、前記第2の抵抗の端子間に与える容量を連続
的に変化させるように構成してある。
(Means for Solving the Problem) In order to achieve the eye movement, the semiconductor laser drive circuit according to the present invention connects a first capacitor between a source electrode of a field effect transistor and a reference potential, and connects the source electrode to the source electrode. A first resistor is connected to a power source, a series circuit of a second resistor and a laser diode is connected between the drain electrode of the field effect transistor and a reference potential, and the second resistor and the laser diode are connected. A laser diode by connecting a DC bias supply circuit to a common connection point of the field effect transistor and a second capacitor connected in parallel with the second resistor, and supplying a pulse current to the gate of the field effect transistor. In a semiconductor laser drive circuit for oscillating a laser, a second field effect transistor is connected in parallel to the second resistor instead of the second capacitor. However, by controlling the gate voltage of the second field effect transistor, the capacitance applied between the terminals of the second resistor is continuously changed.

(実 施 例) 以下、図面を参照して本発明をさらに詳しく説明す
る。
Hereinafter, the present invention will be described in more detail with reference to the drawings.

第1図は本発明による半導体レーザ駆動回路の一実施
例を示す回路図である。
FIG. 1 is a circuit diagram showing an embodiment of a semiconductor laser drive circuit according to the present invention.

図において、1,7は電界効果形トランジスタ(以下FET
と略称する。)、2,4は抵抗器、3はコンデンサ、5は
半導体レーザダイオード、6は直流バイアス供給回路で
ある。
In the figure, 1 and 7 are field effect transistors (hereinafter referred to as FET
Is abbreviated. ), 2 and 4 are resistors, 3 is a capacitor, 5 is a semiconductor laser diode, and 6 is a DC bias supply circuit.

FET1のゲート電極Gにパルス信号が入力されると、入
力パルス信号に応じた駆動パルス電流が得られる。その
駆動パルス電流が半導体レーザダイオード5に注入され
ると半導体レーザダイオード5が発振する。しかしなが
ら半導体レーザダイオード5は1ビツト目のパルスに対
し発振遅延が生じ、発光が遅れるため、パターン効果が
生じ光波形は劣化する。
When a pulse signal is input to the gate electrode G of FET1, a drive pulse current corresponding to the input pulse signal is obtained. When the drive pulse current is injected into the semiconductor laser diode 5, the semiconductor laser diode 5 oscillates. However, the semiconductor laser diode 5 causes an oscillation delay with respect to the pulse of the first bit and delays the light emission, so that the pattern effect occurs and the optical waveform deteriorates.

本発明はこれを補償するために第2のFET7を抵抗4に
並列に接続している。これによりFET7のドレイン−ソー
ス間容量あるいはゲート−ソース間、ゲート−ドレイン
間容量と、抵抗4により駆動パルス電流波形のスピード
をあげるとともに、1ビツト目のパルスにオーバーシユ
ートを持たせている。
The present invention connects a second FET 7 in parallel with the resistor 4 to compensate for this. As a result, the drain-source capacitance of the FET 7, the gate-source capacitance, the gate-drain capacitance, and the resistance 4 increase the speed of the drive pulse current waveform, and the first bit pulse has an overshoot.

一般に高周波領域においては、実装の影響や半導体レ
ーザダイオード5のバラツキが大きいので、パターン効
果による光波形の劣化量は一様ではない。
In general, in the high frequency region, the amount of deterioration of the optical waveform due to the pattern effect is not uniform because the mounting effect and the variation of the semiconductor laser diode 5 are large.

そのため、補償する容量を可変する必要性が生じ、高
周波になればなるほど容量値は小さくなり通常のデイス
クリート部品での実現が困難となる。
Therefore, it becomes necessary to change the capacity to be compensated, and the higher the frequency is, the smaller the capacity value becomes, which makes it difficult to realize the normal discrete component.

本発明では、この光波形補償用の容量を第2のFET7の
ドレイン−ソース間容量あるいは、ゲート−ソース間容
量、およびゲート−ドレイン間容量で実現している。こ
れらの容量は電流の関数になつており、FET7のゲート電
圧を制御することにより、連続的に変えることができ
る。
In the present invention, this capacitance for optical waveform compensation is realized by the drain-source capacitance, the gate-source capacitance, and the gate-drain capacitance of the second FET 7. These capacitances are a function of current, and can be changed continuously by controlling the gate voltage of FET7.

(発明の効果) 以上、説明したように本発明は、電界効果形トランジ
スタのドレイン電極とレーザダイオードとの間の抵抗に
並列接続されたスピードアツプコンデンサの代りに第2
の電界効果形トランジスタを接続し、第2の電界効果形
トランジスタのドレイン−ソース間容量、ゲート−ソー
ス間容量、ゲート−ドレイン間容量をゲート電圧で制御
することにより容量を連続的に変えることが可能とな
り、電圧を変えるだけで容易に光波形を補償し、最適化
できるという効果がある。
(Effects of the Invention) As described above, the present invention is the second embodiment instead of the speed-up capacitor connected in parallel to the resistor between the drain electrode of the field effect transistor and the laser diode.
Of the second field effect transistor is connected, and the capacitance can be continuously changed by controlling the drain-source capacitance, the gate-source capacitance, and the gate-drain capacitance of the second field-effect transistor by the gate voltage. This is possible, and there is an effect that the optical waveform can be easily compensated and optimized simply by changing the voltage.

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

第1図は本発明による半導体レーザ駆動回路の一実施例
を示す回路図、第2図は従来の半導体レーザ駆動回路の
一例を示す図である。 1,7……電界効果形トランジスタ 2,4……抵抗、3,8……コンデンサ 5……半導体レーザダイオード 6……直流バイアス供給回路
FIG. 1 is a circuit diagram showing an embodiment of a semiconductor laser drive circuit according to the present invention, and FIG. 2 is a diagram showing an example of a conventional semiconductor laser drive circuit. 1,7 ...... Field effect transistor 2,4 ...... Resistance, 3,8 ...... Capacitor 5 ...... Semiconductor laser diode 6 ...... DC bias supply circuit

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】電界効果トランジスタのソース電極と基準
電位との間に第1のコンデンサを接続し、前記ソース電
極と電源との間に第1の抵抗を接続し、前記電界効果ト
ランジスタのドレイン電極と基準電位との間に、第2の
抵抗とレーザダイオードの直列回路を接続し、前記第2
の抵抗とレーザダイオードの共通接続点に直流バイアス
供給回路を接続し、さらに前記第2の抵抗と並列に第2
のコンデンサを接続してなり、前記電界効果形トランジ
スタのゲートにパルス電流を供給することにより前記レ
ーザダイオードを発振させる半導体レーザ駆動回路にお
いて、前記第2のコンデンサの代わりに前記第2の抵抗
に並列に第2の電界効果形トランジスタを接続し、前記
第2の電界効果形トランジスタのゲート電圧を制御する
ことにより、前記第2の抵抗の端子間に与える容量を連
続的に変化させることを特徴とする半導体レーザ駆動回
路。
1. A first electrode is connected between a source electrode of a field effect transistor and a reference potential, a first resistor is connected between the source electrode and a power source, and a drain electrode of the field effect transistor. A second resistor and a laser diode in series circuit between the second resistor and the reference potential.
A DC bias supply circuit is connected to a common connection point of the resistor and the laser diode, and a second bias is connected in parallel with the second resistor.
In a semiconductor laser drive circuit that oscillates the laser diode by supplying a pulse current to the gate of the field-effect transistor in parallel with the second resistor instead of the second capacitor. A second field-effect transistor is connected to and the gate voltage of the second field-effect transistor is controlled to continuously change the capacitance applied between the terminals of the second resistor. Semiconductor laser drive circuit.
JP20591688A 1988-08-19 1988-08-19 Semiconductor laser drive circuit Expired - Lifetime JP2684697B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP20591688A JP2684697B2 (en) 1988-08-19 1988-08-19 Semiconductor laser drive circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP20591688A JP2684697B2 (en) 1988-08-19 1988-08-19 Semiconductor laser drive circuit

Publications (2)

Publication Number Publication Date
JPH0254977A JPH0254977A (en) 1990-02-23
JP2684697B2 true JP2684697B2 (en) 1997-12-03

Family

ID=16514872

Family Applications (1)

Application Number Title Priority Date Filing Date
JP20591688A Expired - Lifetime JP2684697B2 (en) 1988-08-19 1988-08-19 Semiconductor laser drive circuit

Country Status (1)

Country Link
JP (1) JP2684697B2 (en)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH08186312A (en) * 1994-12-30 1996-07-16 Sony Corp Laser diode drive circuit
DE19842155B4 (en) 1998-09-15 2005-06-30 Stabilus Gmbh valve means
JP2013110282A (en) * 2011-11-21 2013-06-06 Canon Inc Drive circuit of light-emitting element and light-emitting device
CN110401103B (en) * 2019-07-26 2021-03-23 光梓信息科技(上海)有限公司 Pulse laser driver

Also Published As

Publication number Publication date
JPH0254977A (en) 1990-02-23

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