JPS63200630A - Optical transmitter-receiver - Google Patents

Optical transmitter-receiver

Info

Publication number
JPS63200630A
JPS63200630A JP62032556A JP3255687A JPS63200630A JP S63200630 A JPS63200630 A JP S63200630A JP 62032556 A JP62032556 A JP 62032556A JP 3255687 A JP3255687 A JP 3255687A JP S63200630 A JPS63200630 A JP S63200630A
Authority
JP
Japan
Prior art keywords
pulse
light
pulse width
optical
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.)
Pending
Application number
JP62032556A
Other languages
Japanese (ja)
Inventor
Kazumasa Tsukada
和正 塚田
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 JP62032556A priority Critical patent/JPS63200630A/en
Publication of JPS63200630A publication Critical patent/JPS63200630A/en
Pending legal-status Critical Current

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  • Dc Digital Transmission (AREA)
  • Optical Communication System (AREA)

Abstract

PURPOSE:To transmit/receive an optical signal with high quality by decreasing the time rate of the emission of a light emitting element to increase the light peak output and eliminating a low frequency zone having much invaded light component. CONSTITUTION:A pulse generating circuit 2 outputs a pulse C<+> having a pulse width t1 based on an input of a leading signal B<+> and a pulse generating circuit 3 outputs a pulse C<-> of a pulse width t2 (t1>t2) based on the trailing B<-> input. In this case, the pulse C<-> is a pulse having a pulse width t2 with a delay of t1-t2 with respect to the B<-> reference. The pulses C<+>, C<-> are synthesized and inputted to an electrooptical conversion circuit 5 as a transmission pulse D and converted into an optical pulse D'. Moreover, the time rate of pulse emission of the pulse D to the sent data A by selecting the minimum pulse width of the sent data as Tmin and selecting the relation of t1+t2<Tmin and the peak output of light is increased by the reduction of the time rate. Furthermore, the pulse D' is converted into an electric signal D'' by an optoelectric conversion circuit 6 and a low frequency component including much invaded light component is eliminated by a differentiation circuit 7.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は光の空間伝送に適する光送受信器に関する。[Detailed description of the invention] [Industrial application field] The present invention relates to an optical transceiver suitable for spatial transmission of light.

し従来の技術〕 光強度変調による光の空間伝送において、最とも大きな
障害は太陽光などの自然光及び照明等の人工光の光受信
器への混入である。これらの混入は雑音として受信され
ることになるために、できるだけ除去することが望まし
い。雑音除去の方法としては信号光の波長帯域以外の波
長領域の光を光ろ波器により除去する方法及び電気信号
に変換後信号成分以外を沖波器で除去する方法がある。
[Prior Art] In the spatial transmission of light by light intensity modulation, the most serious obstacle is the contamination of natural light such as sunlight and artificial light such as lighting into an optical receiver. Since these contaminations are received as noise, it is desirable to remove them as much as possible. Methods of noise removal include a method in which light in a wavelength range other than the wavelength band of the signal light is removed by an optical filter, and a method in which after conversion to an electrical signal, components other than the signal components are removed by an optical wave filter.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

雑音は光領域での除去が最とも望ましい方法であるが、
混入光の中に信号光と同波長成分が存在すること、信号
光以外の成分を効率よく除去するF波特性を持たせると
高価になる等の問題がある。
The most desirable way to remove noise is in the optical domain, but
There are problems such as the presence of a component of the same wavelength as the signal light in the mixed light, and the high cost of providing F-wave characteristics that efficiently remove components other than the signal light.

また、電気信号領域で雑音成分を除去する方法としては
、送信データ信号をあらかじめ搬送波を使用して、混入
光の電気信号成分が少ない高域に信号成分を上げて送信
し、受信側で信号成分を沖波器により抽出する方法があ
る。
In addition, as a method for removing noise components in the electrical signal domain, the transmitted data signal is transmitted in advance by using a carrier wave to raise the signal component to a high frequency range where the electrical signal component of the mixed light is small, and then the signal component is removed on the receiving side. There is a method of extracting it using an Okinawa device.

更に、混入光からの信号光分離の他の方法として混入光
よりも信号光を強くする方法がある。これによれば信号
光の送信出力が高くできるので最とも容易な解決策とな
る。また、前述の対策を共用すれば更j(受信特性が改
善できる。発光素子として使用される発光ダイオード等
は、一般的に発光時間率を下げる和光のピーク出力を上
げることが可能であシ、キーク出力を高くすることによ
って混入光よりも高い信号光として受信することが可能
となる。
Furthermore, as another method for separating signal light from mixed light, there is a method of making the signal light stronger than the mixed light. According to this method, the transmission power of the signal light can be increased, which is the easiest solution. In addition, if the above-mentioned countermeasures are used in common, the reception characteristics can be further improved.It is possible to increase the peak output of the light emitting diode used as a light emitting element, which generally reduces the light emitting time rate. By increasing the key output, it becomes possible to receive signal light that is higher than the mixed light.

本発明の目的は、送信側で発光素子の発光時間率を下げ
る手段を構することによって光のピーク出力を上げると
ともに、受信側では混入光成分の多い低周波領域を除去
することによって2品質のよい光信号を送受することの
できる光送受信器を提供することにある。
The purpose of the present invention is to increase the peak output of light by providing means for reducing the light emission time rate of the light emitting element on the transmitting side, and to improve the quality of the two-quality light by removing the low frequency region with many mixed light components on the receiving side. An object of the present invention is to provide an optical transceiver capable of transmitting and receiving good optical signals.

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

本発明による光送受信器は、送信データパルスの立上シ
及び立下りを検出する手段と、立上りに対して送信デー
タパルスの最小パルス幅Tminの1/2より小さいパ
ルス幅t、のパルスを発生し、立下シに対して前記Tm
inの1/2より小さく前記t1と異った値のパルス幅
t2のパルスを発生する手段とヲ備工、前記パルス幅t
、のパルスの立下りとパルス幅t2のパルスの立下りの
時間間隔が送信データパルスのパルス幅に等しくなるよ
うに結合したのち光A?ルスに変換する光送信器と、光
信号から変換された電気信号パルスを微分する手段と、
該微分された信号の立上り部分から立下シ部分までの時
間間隔を計測する手段とを備え、その時間間隔が実質的
にt、であれば送信データパルスの立上りと判定し、実
質的にt2であれば送信データパルスの立下りと判定し
て、立上り判定により二安定回路をセットし、立下シ判
定により前記二安定回路をリセットする光受信器とを含
むことを特徴とする。
The optical transceiver according to the present invention includes means for detecting the rising edge and falling edge of a transmitted data pulse, and generates a pulse having a pulse width t smaller than 1/2 of the minimum pulse width Tmin of the transmitted data pulse with respect to the rising edge. Then, the Tm
Means and equipment for generating a pulse having a pulse width t2 smaller than 1/2 of in and different from the t1, and the pulse width t
, and the time interval between the falling edge of the pulse with pulse width t2 is equal to the pulse width of the transmission data pulse, and then the light A? an optical transmitter for converting the electrical signal pulse into a signal; and a means for differentiating the electrical signal pulse converted from the optical signal.
means for measuring the time interval from the rising edge to the falling edge of the differentiated signal, and if the time interval is substantially t, it is determined that it is the rising edge of the transmission data pulse, and the time interval is substantially t2. If so, the optical receiver determines that the transmission data pulse is falling, sets a bistable circuit based on the rising edge determination, and resets the bistable circuit based on the falling edge determination.

る。Ru.

〔実施例〕〔Example〕

次に2本発明について図面を参照して説明する。 Next, two aspects of the present invention will be explained with reference to the drawings.

第1図は本発明による光送受信器の実施例の構成を示す
ブロック図、第2図は、第1図の実施例の動作を示す各
部波形図である。これ等の図において、送信データAが
立上り、立下り分離回路1に入力し、そのデータパルス
の立上り部分を検出し、立上多信号B+とじてパルス発
生回路2に入力する。同様に、データパルスの立下り部
分を検出し、立下多信号B−としてパルス発生回路3に
入力する。
FIG. 1 is a block diagram showing the configuration of an embodiment of an optical transceiver according to the present invention, and FIG. 2 is a waveform diagram of each part showing the operation of the embodiment of FIG. In these figures, transmission data A is input to a rising and falling separation circuit 1, and the rising portion of the data pulse is detected and input to a pulse generation circuit 2 as a rising multi-signal B+. Similarly, the falling portion of the data pulse is detected and inputted to the pulse generation circuit 3 as the falling multi-signal B-.

第1図のパルス発生回路2では立上多信号B入力を基準
としてパルス幅t1の・やルスCを出力する。
The pulse generating circuit 2 shown in FIG. 1 outputs a pulse C having a pulse width t1 with reference to the rising edge multi-signal B input.

第1図のパルス発生回路3では、立下シ信号B−人力を
基準としてパルス幅t2(t、〉t2)のパルスC−を
出力する。なお、この場合、C−はB−基準に対しく5
) て1.−12時間遅れたパルス幅t2のパルスとする。
The pulse generating circuit 3 in FIG. 1 outputs a pulse C- having a pulse width t2 (t,>t2) with reference to the falling signal B-human power. In addition, in this case, C- is 5 against the B- standard.
) te1. - The pulse has a pulse width t2 delayed by 12 hours.

C+、C−は第1図の結合回路4において合成され。C+ and C- are combined in the coupling circuit 4 of FIG.

送信パルスDとして電気−光変換回路5に入力さ:h 
# 光ノ’?ルスD’に変換サレる。C+パルストc−
パルスの立下シ時点の間隔はパルス発光回路3において
C−a4ルスをtl−t2時間遅らせたことにより送信
データのパルス幅に等しい間隔となっている。
Input to the electro-optical conversion circuit 5 as a transmission pulse D: h
# Light'? Convert to Luz D'. C+Pulst c-
The interval between the falling points of the pulse is equal to the pulse width of the transmission data because the C-a4 pulse is delayed by tl-t2 time in the pulse light emitting circuit 3.

また、送信データの最小パルス幅をTminとし。Also, let Tmin be the minimum pulse width of transmission data.

t1+t2〈Tmin となシ、送信データAに対して
送信パルスDのパルス発生の時間率が下がることになり
、この時間率の低下分だけ光のピーク出力を高めること
が可能となる。
As t1+t2<Tmin, the pulse generation time rate of the transmission pulse D with respect to the transmission data A decreases, and it becomes possible to increase the peak output of light by the decrease in the time rate.

第1図および第2図におけるD′の光送信パルスは空間
伝送路を経て光−電気変換回路6において電気信号D“
に変換される。この電気信号DIは微分回路7において
混入光成分の多い低周波成分が除去され、微分波Eとし
て時間間隔計測回路8および9に入力する。
The optical transmission pulse D' in FIGS.
is converted to This electrical signal DI is subjected to a differentiation circuit 7 in which low frequency components with many mixed optical components are removed, and is input as a differential wave E to time interval measurement circuits 8 and 9.

時間間隔計測回路8は微分波Eの(+)微分から←)微
分の間隔がt、±Δ1 / (Δt′は判定許容範囲)
の範囲にある時、F信号を出力する。同様に時間間隔計
測回路9は微分波Eの(+)微分から(→微分の間隔が
t2±Δt// (Δt〃は判定許容範囲)の範囲にあ
る時。
The time interval measuring circuit 8 calculates the (+) differential of the differential wave E from the (←) differential interval to t, ±Δ1/(Δt' is the judgment tolerance range)
When it is within the range of , the F signal is output. Similarly, the time interval measurement circuit 9 detects the (+) differential of the differential wave E when the differential interval is within the range of t2±Δt// (Δt is the permissible judgment range).

F−信号を出力する。すなわち、F信号はパルス幅t(
7)d’ルス、rはノ9ルス幅t2のパルスを受信した
ものと判定し、その判定出力は(→微分の終了時点とな
るため、その位置においてF+、又はF−信号が出力さ
れる。F は送信データの立上りに相当し。
Output F-signal. That is, the F signal has a pulse width t(
7) d'rus and r are determined to have received a pulse with a width of t2, and the determination output is (→ Since this is the end point of differentiation, an F+ or F- signal is output at that position. .F corresponds to the rising edge of the transmitted data.

F−は立下シに相当するため、フリップフロップ回路1
0をF+でセットし、F−信号でリセットすることによ
って出力側に再生送信データGが得られる。
Since F- corresponds to the falling edge, the flip-flop circuit 1
By setting 0 with F+ and resetting with F- signal, reproduced transmission data G is obtained on the output side.

〔発明の効果〕〔Effect of the invention〕

以上の説明により明らかなように2本発明によれば9発
光素子の発光時間率が下がることによって光ピーク出力
を上げ、また受信信号を微分することによって混入光成
分を低減させ得る効果がある。
As is clear from the above description, the present invention has the effect of increasing the optical peak output by lowering the light emission time rate of the nine light emitting elements, and reducing mixed light components by differentiating the received signal.

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

第1図は本発明による実施例の構成を示すブロック図、
第2図は第1図の実施例における各部の動作波形を示す
タイムチャートである。図において、lは立上シ、立下
シ分離回路、2,3はパルス発生回路、4は結合回路、
5は電気−光変換回路、6は光−電気変換回路、7は微
分回路、8゜9は時間間隔計測回路、10はフリップフ
ロップ回路である。 第1図 拮2図
FIG. 1 is a block diagram showing the configuration of an embodiment according to the present invention;
FIG. 2 is a time chart showing operating waveforms of each part in the embodiment of FIG. 1. In the figure, l is a rising edge and falling edge separation circuit, 2 and 3 are pulse generation circuits, 4 is a coupling circuit,
5 is an electric-to-optical conversion circuit, 6 is an optical-to-electrical conversion circuit, 7 is a differential circuit, 8.9 is a time interval measuring circuit, and 10 is a flip-flop circuit. Figure 1 Figure 2

Claims (1)

【特許請求の範囲】[Claims] 1、送信データパルスの立上り及び立下りを検出する手
段と、立上りに対して送信データパルスの最小パルス幅
T_m_i_nの1/2より小さいパルス幅を、のパル
スを発生し、立下りに対して前記T_m_i_nの1/
2より小さく前記t_1と異った値のパルス幅t_2の
パルスを発生する手段とを備え、前パルス幅を、のパル
スの立下りとパルス幅t_2のパルスの立下りの時間間
隔が送信データパルスのパルス幅に等しくなるように結
合したのち光パルスに変換する光送信器と、光信号から
変換された電気信号パルスを微分する手段と、該微分さ
れた信号の立上り部分から立下り部分までの時間間隔を
計測する手段とを備え、その時間間隔が実質的にt_1
であれば送信データパルスの立上りと判定し、実質的に
t_2であれば送信データパルスの立下りと判定して、
立上り判定により二安定回路をセットし、立下り判定に
より前記二安定回路をリセットする光受信器とを含むこ
とを特徴とする光送受信器。
1. Means for detecting the rising and falling edges of a transmission data pulse; generating a pulse having a pulse width smaller than 1/2 of the minimum pulse width T_m_i_n of the transmission data pulse for a rising edge; 1/ of T_m_i_n
means for generating a pulse with a pulse width t_2 smaller than 2 and different from said t_1, and the time interval between the falling edge of the pulse and the falling edge of the pulse with the pulse width t_2 is the transmission data pulse. an optical transmitter that converts the electrical signal pulses into optical pulses after combining them so that the pulse width is equal to the pulse width of the optical signal; a means for differentiating the electrical signal pulses converted from the optical signals; means for measuring a time interval, the time interval being substantially t_1.
If so, it is determined that it is the rising edge of the transmission data pulse, and if it is substantially t_2, it is determined that it is the falling edge of the transmission data pulse.
An optical transmitter/receiver comprising: an optical receiver that sets a bistable circuit based on a rise determination, and resets the bistable circuit based on a fall determination.
JP62032556A 1987-02-17 1987-02-17 Optical transmitter-receiver Pending JPS63200630A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62032556A JPS63200630A (en) 1987-02-17 1987-02-17 Optical transmitter-receiver

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62032556A JPS63200630A (en) 1987-02-17 1987-02-17 Optical transmitter-receiver

Publications (1)

Publication Number Publication Date
JPS63200630A true JPS63200630A (en) 1988-08-18

Family

ID=12362188

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62032556A Pending JPS63200630A (en) 1987-02-17 1987-02-17 Optical transmitter-receiver

Country Status (1)

Country Link
JP (1) JPS63200630A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04263309A (en) * 1991-02-18 1992-09-18 Matsushita Electric Ind Co Ltd Optically coupled terminal equipment
WO1997016889A1 (en) * 1995-10-30 1997-05-09 Smk Corporation Pulse modulating method, pulse modulator, and pulse demodulator

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04263309A (en) * 1991-02-18 1992-09-18 Matsushita Electric Ind Co Ltd Optically coupled terminal equipment
WO1997016889A1 (en) * 1995-10-30 1997-05-09 Smk Corporation Pulse modulating method, pulse modulator, and pulse demodulator

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