JPH0327633A - Laser diode driving system - Google Patents

Laser diode driving system

Info

Publication number
JPH0327633A
JPH0327633A JP1162041A JP16204189A JPH0327633A JP H0327633 A JPH0327633 A JP H0327633A JP 1162041 A JP1162041 A JP 1162041A JP 16204189 A JP16204189 A JP 16204189A JP H0327633 A JPH0327633 A JP H0327633A
Authority
JP
Japan
Prior art keywords
signal
circuit
nrz
laser diode
base
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.)
Pending
Application number
JP1162041A
Other languages
Japanese (ja)
Inventor
Hiroo Kitasagami
北相模 博夫
Takashi Tsuda
津田 高至
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.)
Fujitsu Ltd
Original Assignee
Fujitsu 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 Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP1162041A priority Critical patent/JPH0327633A/en
Publication of JPH0327633A publication Critical patent/JPH0327633A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To output an NRZ optical signal whose half value width is 100% by taking logic operation to a retarded NRZ signal and the original NRZ signal and inputting a signal whose half value width is increased by 100% or above to the driving circuit of a laser diode. CONSTITUTION:A variable delay circuit 1 retards an inputted NRZ electric signal for an optical time and is connected to the 2nd input terminal of an OR circuit 2. A laser diode LD 3 emits a coherent light with the strength responding to the current to be inputted, the output terminal of the circuit 2 is connected to an LD driving circuit 4 driving the LD 3. The circuit 4 is a differential current switching circuit, an NRZ signal is inputted to the base of one TR 1 and a voltage VREF1 being the center level of the NRZ signal inputted to the base of the TR 1 is fed to the base of other TR 2. A 3rd TR 3 is a TR to supply a bias current and the voltage VREF2 to set the bias current is applied to the base.

Description

【発明の詳細な説明】 〔概要〕 光通信システムにおいて、NRZのディジタル電気信号
を光信号に変換するためのレーザダイオ一ド駆動方式に
関し、 半値幅100%のNRZ光信号を出力させることができ
るレーザダイオード駆動方式を提供することを目的とし
、 NRZの電気信号を入力してその信号を可変遅延して出
力する可変遅延回路と、上記可変遅延回路の出力信号と
もとの信号との論理をとって、半値幅を100%以上に
増加させた電気信号を出力する論理回路とを設け、電気
信号を光信号に変換するレーザダイオードの駆動回路に
上記論理回路の出力信号を入力させるように構成する。
[Detailed Description of the Invention] [Summary] Regarding a laser diode driving method for converting an NRZ digital electrical signal into an optical signal in an optical communication system, a laser capable of outputting an NRZ optical signal with a half width of 100% is provided. The purpose is to provide a diode drive system, and it is designed by using a variable delay circuit that inputs an NRZ electrical signal and outputs the signal with a variable delay, and by taking the logic between the output signal of the variable delay circuit and the original signal. , and a logic circuit that outputs an electrical signal with a half-width increased to 100% or more, and the output signal of the logic circuit is configured to be input to a laser diode drive circuit that converts the electrical signal into an optical signal.

〔産業上の利用分野〕[Industrial application field]

この発明は、光通信システムにおいて、NRZ(ノンリ
ターンツーゼロ)のディジタル電気信号を光信号に変換
するためのレーザダイオード駆動方式に関する。
The present invention relates to a laser diode driving method for converting an NRZ (non-return-to-zero) digital electrical signal into an optical signal in an optical communication system.

光通信システムの光信号送信器においては、電気信号に
よってレーザダイオードを駆動して、電気信号と同じ波
形のコヒーレントな光信号に変換している。
In an optical signal transmitter of an optical communication system, a laser diode is driven by an electrical signal and converted into a coherent optical signal having the same waveform as the electrical signal.

〔従来の技術〕[Conventional technology]

NRZの電気信号でレーザダイオードを駆動する場合、
NRZ信号のデューティは100%であるから、半値幅
(その信号伝送路のクロツク周期幅に対する、信号波形
の振幅の半分の高さにおけるその波形の幅)が100%
の電気信号で駆動していた。
When driving a laser diode with an NRZ electrical signal,
Since the duty of the NRZ signal is 100%, the half-width (width of the signal waveform at half the height of the amplitude of the signal waveform with respect to the clock cycle width of the signal transmission path) is 100%.
It was driven by electrical signals.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

第4図は、レーザダイオードの駆動電流と光出力との関
係を示している。駆動電流Iがしきい値I lmを越え
ると、その点以上では、光出力はほぼ直線的に増加する
。したがって、そのしきい値に相当するバイアス電流を
与えておけば、電気信号と同じ波形の光出力が得られる
FIG. 4 shows the relationship between the drive current of the laser diode and the optical output. Once the drive current I exceeds the threshold I lm, the light output increases approximately linearly above that point. Therefore, if a bias current corresponding to the threshold value is applied, an optical output having the same waveform as the electrical signal can be obtained.

しかし、実際には、消光比を良くして、信号の「0」レ
ベルでの発光を確実に無くすために、バイアス電流I,
はしきい値電流■.より少し小さく設定され、そこを基
貼として信号電流によって駆動される。その結果、光出
力の半値幅Bは、電気信号の半値幅Aより小さくなる。
However, in reality, in order to improve the extinction ratio and reliably eliminate light emission at the "0" level of the signal, the bias current I,
is the threshold current ■. It is set a little smaller than that, and is driven by a signal current based on that point. As a result, the half-width B of the optical output becomes smaller than the half-width A of the electrical signal.

このような駆動方式において、従来は、半値幅100%
のNRZ電気信号でレーザダイオードを駆動していたの
で、光出力の半値幅が100%に達しなくなってしまう
問題があった。半値幅が100%に達しないと、信号デ
ータが「1」のときのデューティが小さくなって、アイ
パターン波形のクロス点がずれてしまう等、光信号の規
格に適合しない波形になってしまう。
In such a drive system, conventionally, the half width is 100%.
Since the laser diode was driven by the NRZ electric signal, there was a problem in that the half width of the optical output did not reach 100%. If the half-value width does not reach 100%, the duty when the signal data is "1" becomes small, and the cross point of the eye pattern waveform shifts, resulting in a waveform that does not conform to the optical signal standard.

この発明は、゜そのような従来の欠点を解消し、半値幅
100%のNRZ光信号を出力させることができるレー
ザダイオード駆動方式を提供することを目的とする。
It is an object of the present invention to provide a laser diode driving system capable of eliminating such conventional drawbacks and outputting an NRZ optical signal with a half width of 100%.

〔課題を解決するための手段〕[Means to solve the problem]

上記の目的を達成するため、本発明のレーザダイオード
駆動方式は、第1図に示されるように、NRZの電気信
号を人力してその信号を可変遅延して出力する可変遅延
回路lと、上記可変遅延回路lの出力信号ともとの信号
との論理をとって、半値幅を100%以上に増加させた
電気信号を出力する論理回路2とを設け、電気信号を光
信号に変換するレーザダイオード3の駆動回路4に上記
論理回路2の出力信号を人力させることを特徴とする。
In order to achieve the above object, the laser diode driving method of the present invention, as shown in FIG. A laser diode that converts the electrical signal into an optical signal by providing a logic circuit 2 that takes the logic between the output signal of the variable delay circuit 1 and the original signal and outputs an electrical signal whose half width is increased to 100% or more. It is characterized in that the output signal of the logic circuit 2 is manually input to the drive circuit 4 of No. 3.

〔作用〕[Effect]

可変遅延回路1で遅延されたNRZ電気信号ともとのN
RZ電気信号との論理をとって、半値幅が100%以上
に増加した電気信号が、論理回路2からレーザダイオー
ド3の駆動回路4に人力する。したがって、光出力の半
値幅が電気信号の半値幅より小さくても、光出力の半値
幅を100%にすることができる。この際に、可変遅延
回路lでNRZ電気信号の遅延量を変えることによって
、駆動回路4に人力するNRZ電気信号の半値幅を調整
し、光出力の半値幅をちょうど100%にすることがで
きる。
The NRZ electric signal delayed by the variable delay circuit 1 and the original N
Based on the logic with the RZ electric signal, an electric signal whose half width has increased to 100% or more is input from the logic circuit 2 to the drive circuit 4 of the laser diode 3. Therefore, even if the half-width of the optical output is smaller than the half-width of the electrical signal, the half-width of the optical output can be made 100%. At this time, by changing the amount of delay of the NRZ electrical signal using the variable delay circuit 1, the half-width of the NRZ electrical signal inputted to the drive circuit 4 can be adjusted, and the half-width of the optical output can be made exactly 100%. .

〔実施例〕〔Example〕

図面を参照して実施例を説明する。 Examples will be described with reference to the drawings.

第2図において、IOは、NRZ電気信号の入力端であ
り、分岐されて、公知の可変遅延回路1とOR回路2の
第1の人力端のとに接続されている。
In FIG. 2, IO is an input terminal for the NRZ electrical signal, which is branched and connected to a known variable delay circuit 1 and a first input terminal of an OR circuit 2.

可変遅延回路lは、人力されたNRZの電気信号を任意
時間遅延させて出力し、その出力端はOR回路2の第2
の入力端■に接続されている。
The variable delay circuit 1 delays the human-powered NRZ electric signal by an arbitrary time and outputs it, and its output terminal is connected to the second terminal of the OR circuit 2.
Connected to the input terminal ■.

3は、人力される電流値に応じた強さのコヒーレント光
を発光するレーザダイオード(LD)であり、OR回路
2の出力端■は、LD3を駆動するための公知のLD駆
動回路4に接続されている。
3 is a laser diode (LD) that emits coherent light whose intensity corresponds to the current value manually applied, and the output terminal (■) of the OR circuit 2 is connected to a known LD drive circuit 4 for driving the LD 3. has been done.

本実施例において、LD駆動回路4は差動型の電流スイ
ッチング回路であり、同特性の2つのトランジスタTR
I,TR2が用いられている。そして、一方のトランジ
スタTRIのベースにNRZ信号が入力され、他方のト
ランジスタTR2のベースには、TRIのベースに入力
されるNRZ信?の中心電位となる電圧■1l1,Iが
かけられている。
In this embodiment, the LD drive circuit 4 is a differential current switching circuit, and has two transistors TR with the same characteristics.
I,TR2 is used. The NRZ signal is input to the base of one transistor TRI, and the NRZ signal input to the base of TRI is input to the base of the other transistor TR2. A voltage ■1l1,I, which is the center potential of , is applied.

また、第3のトランジスタTR3はバイアス電流を供給
するためのトランジスタであり、そのべ−スに、バイア
ス電流を設定するための電圧V■..2がかけられてい
る。このバイアス電流I,はLD3のしきい値電流I.
より少し小さく、前述した第4図に示されるように、L
D3の光出力波形の半値幅Bは、電気信号波形の半値幅
Aより少し狭くなっている。
Further, the third transistor TR3 is a transistor for supplying a bias current, and has a base voltage V1.0 for setting the bias current. .. 2 is applied. This bias current I, is the threshold current I. of LD3.
It is slightly smaller than L, as shown in FIG.
The half-width B of the optical output waveform of D3 is slightly narrower than the half-width A of the electrical signal waveform.

このように構成された実施例においては、OR回路2に
よって、電気信号の半値幅が100%以上に増加してL
D駆動回路4に入力する。第3図はその状態を示すタイ
ムチャートであり、OR回路2の出力端■へ出てくる信
号は、各入力端の,■への入力信号の論理和となってお
り、その結果、連続する“l”の範囲ごとにその幅が拡
がり、出力端の信号■の半値幅が100%以上となる。
In the embodiment configured in this way, the half width of the electrical signal is increased to 100% or more by the OR circuit 2, and L
Input to D drive circuit 4. Figure 3 is a time chart showing this state, and the signal that comes out to the output terminal (■) of the OR circuit 2 is the logical sum of the input signals to (■) of each input terminal, and as a result, the signal that comes out to the output terminal (■) of the OR circuit 2 is the The width increases for each range of "1", and the half width of the signal (2) at the output end becomes 100% or more.

そして、このLD駆動回路4に入力する電気信号の半値
幅は、可変遅延回路1の遅延量を調整することによって
変えることができる。そして、LD3からの光出力信号
のアイパターン波形を見ながら、その波形が最も好まし
い状態、即ち、光信号波形の半値幅が100%になるよ
うに調整することができる。
The half-value width of the electrical signal input to the LD drive circuit 4 can be changed by adjusting the delay amount of the variable delay circuit 1. Then, while looking at the eye pattern waveform of the optical output signal from the LD 3, it is possible to adjust the waveform so that it is in the most desirable state, that is, the half width of the optical signal waveform is 100%.

なお、論理回路として上記実施例ではOR回路を用いた
が、負論理をとることにより、論理積を用いるAND回
路を用いても全く同じ結果を得ることができる。
Although an OR circuit is used as the logic circuit in the above embodiment, the exact same result can be obtained by using an AND circuit using logical product by taking negative logic.

〔発明の効果〕〔Effect of the invention〕

本発明のレーザダイオード駆動方式によれば、半値幅が
100%の光信号を容易に出力させることができるので
、規格に適合する良好な波形の光信号を常に安定して得
ることができる優れた効果を有する。
According to the laser diode drive method of the present invention, it is possible to easily output an optical signal with a half-width of 100%, so it is an excellent method that can always stably obtain an optical signal with a good waveform that conforms to the standard. have an effect.

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

第1図は本発明の原理図、 第2図は実施例の回路図、 第3図は論理回路の入出力信号タイムチャート図、 第4図は駆動電流対光出力特性線図である。 図中、■・・・可変遅延回路、 2・・・論理回路、 3・・・レーザダイオード、 4・・・駆動回路。 −21 Figure 1 is a diagram of the principle of the present invention. Figure 2 is a circuit diagram of the embodiment, Figure 3 is a logic circuit input/output signal time chart, FIG. 4 is a drive current versus light output characteristic diagram. In the figure, ■...variable delay circuit, 2...logic circuit, 3...Laser diode, 4... Drive circuit. -21

Claims (1)

【特許請求の範囲】 NRZの電気信号を入力してその信号を可変遅延して出
力する可変遅延回路(1)と、 上記可変遅延回路(1)の出力信号ともとの信号との論
理をとって、半値幅を100%以上に増加させた電気信
号を出力する論理回路(2)とを設け、 電気信号を光信号に変換するレーザダイオード(3)の
駆動回路(4)に上記論理回路(2)の出力信号を入力
させることを 特徴とするレーザダイオード駆動方式。
[Claims] A variable delay circuit (1) that inputs an NRZ electrical signal and outputs the signal with a variable delay, and a logic circuit between the output signal of the variable delay circuit (1) and the original signal. A logic circuit (2) that outputs an electrical signal with a half width increased to 100% or more is provided, and a drive circuit (4) for a laser diode (3) that converts the electrical signal into an optical signal is provided with the logic circuit (2). A laser diode drive method characterized by inputting the output signal of 2).
JP1162041A 1989-06-23 1989-06-23 Laser diode driving system Pending JPH0327633A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1162041A JPH0327633A (en) 1989-06-23 1989-06-23 Laser diode driving system

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1162041A JPH0327633A (en) 1989-06-23 1989-06-23 Laser diode driving system

Publications (1)

Publication Number Publication Date
JPH0327633A true JPH0327633A (en) 1991-02-06

Family

ID=15746966

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1162041A Pending JPH0327633A (en) 1989-06-23 1989-06-23 Laser diode driving system

Country Status (1)

Country Link
JP (1) JPH0327633A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2006201096A (en) * 2005-01-24 2006-08-03 Otis Elevator Co Vibration detector

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2006201096A (en) * 2005-01-24 2006-08-03 Otis Elevator Co Vibration detector

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