JPS6139775B2 - - Google Patents
Info
- Publication number
- JPS6139775B2 JPS6139775B2 JP54001203A JP120379A JPS6139775B2 JP S6139775 B2 JPS6139775 B2 JP S6139775B2 JP 54001203 A JP54001203 A JP 54001203A JP 120379 A JP120379 A JP 120379A JP S6139775 B2 JPS6139775 B2 JP S6139775B2
- Authority
- JP
- Japan
- Prior art keywords
- optical
- signal
- output
- input
- transmission
- 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
Links
- 230000003287 optical effect Effects 0.000 claims description 38
- 230000005540 biological transmission Effects 0.000 claims description 18
- 238000000295 emission spectrum Methods 0.000 claims description 2
- 239000004065 semiconductor Substances 0.000 description 17
- 239000000835 fiber Substances 0.000 description 9
- 238000010586 diagram Methods 0.000 description 4
- 230000010355 oscillation Effects 0.000 description 4
- 238000001228 spectrum Methods 0.000 description 4
- 238000006243 chemical reaction Methods 0.000 description 2
- 239000000969 carrier Substances 0.000 description 1
- 230000002542 deteriorative effect Effects 0.000 description 1
- 230000003595 spectral effect Effects 0.000 description 1
- 238000000411 transmission spectrum Methods 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04J—MULTIPLEX COMMUNICATION
- H04J14/00—Optical multiplex systems
- H04J14/02—Wavelength-division multiplex systems
- H04J14/0298—Wavelength-division multiplex systems with sub-carrier multiplexing [SCM]
Landscapes
- Engineering & Computer Science (AREA)
- Computer Networks & Wireless Communication (AREA)
- Signal Processing (AREA)
- Optical Communication System (AREA)
Description
【発明の詳細な説明】
現在、強度変調の長距離光伝送を行う場合高出
力の半導体レーザーが一般に使用されている。半
導体レーザは電流対光出力特性の直線性が悪く光
周波数多重を行う場合その非直線性による混変調
や相互変調によるビート妨害の発生が問題とな
る。しかも半導体レーザの電流対光出力特性の直
線性がロツトにより左右され、その結果、多重す
るチヤネル数が規制されてしまう。この様に伝送
するチヤネル数が半導体レーザのロツトにより左
右されている現状では、システム設計が非常に難
しく、場合によつては、伝送チヤネルを減少させ
るか又は、半導体レザの製造段階で直線性の良い
ものが得られるまで待たねばならぬ事態が生じて
くる。DETAILED DESCRIPTION OF THE INVENTION Currently, high-output semiconductor lasers are generally used for intensity modulated long-distance optical transmission. Semiconductor lasers have poor linearity in current vs. optical output characteristics, and when performing optical frequency multiplexing, problems arise in the occurrence of beat disturbances due to cross modulation and intermodulation due to the nonlinearity. Moreover, the linearity of the current vs. optical output characteristic of the semiconductor laser is affected by the lot, and as a result, the number of multiplexed channels is restricted. Currently, the number of transmission channels is determined by the number of semiconductor laser lots, making system design extremely difficult. Situations arise where you have to wait until you get something good.
本発明は上記問題を解決するもので、半導体レ
ーザの特性のバラツキに影響されず、したがつて
多重伝送に非常に有用な優れた伝送方式を提供す
るものである。以下その一実施例を図面に基づい
て説明する。 The present invention solves the above problems and provides an excellent transmission system that is not affected by variations in the characteristics of semiconductor lasers and is therefore very useful for multiplex transmission. One embodiment will be described below based on the drawings.
第1図は本方式の装置の一例でまず複数個の混
合された搬送波が端子1に入力される。この信号
は帯域通過波器で構成された分波器2により分
波され、その分波された個々の搬送波信号が、発
光スペクトル波長のそれぞれλ1,λ2……λo
と異なる半導体レーザ3に入力され電気―光の変
換が行われる。ここで強度変調された光出力信号
はそれぞれ専用のフアイバ4で結合され、グレー
テイング、又は誘電体多層膜等を利用した光合成
器5に入力される。光合成器5の光通過領域の中
心波長は前段の半導体レーザの発振スペクトル波
長λ1,λ2……λoと一致しているため出力は
光フイルタによつて混合された光信号となる。そ
してそれぞれの強度変調された光信号は光合成器
5の出力から一本の伝送フアイバ6により送出さ
れる。送出された光信号は光合成器5の装置と同
じ構成で入出力端子のみを逆接続した光分波器7
に入力される。この光入力信号は発振波長がそれ
ぞれ異なる半導体レーザにより強度変調されてい
るため、光分波器7により分波されそれぞれの受
光素子9により光―電気変換が行われる。ここま
で伝送された光信号は半導体レーザの電流対光出
力特性の非直線性により、基本波全分の2倍、3
倍という2次、3次ビート歪が生じており、信号
の質が劣化している。受光素子により変換され歪
をもつた電気信号は帯域通過波器で構成された
混合器10により高調波歪が除去される。ここで
混合器10は分波器2と同様に搬送波の中心周波
数に設定されている。そして、それぞれ基本波の
みの電気信号が端子11に得られる。このように
発光素子等で生じた高調波成分を電気系で除去す
るため非常に簡単に構成できる。 FIG. 1 shows an example of a device using this system, in which a plurality of mixed carrier waves are input to terminal 1. This signal is demultiplexed by a demultiplexer 2 composed of a bandpass waveform, and the demultiplexed carrier signals are divided into wavelengths of the emission spectrum λ 1 , λ 2 . . . λ o
The light is input to a different semiconductor laser 3 and electrical-to-optical conversion is performed. Here, the intensity-modulated optical output signals are combined through dedicated fibers 4, and input to a light combiner 5 using a grating, a dielectric multilayer film, or the like. Since the center wavelength of the light passing region of the optical combiner 5 coincides with the oscillation spectrum wavelengths λ 1 , λ 2 , . Each intensity-modulated optical signal is sent out from the output of the optical combiner 5 through one transmission fiber 6. The transmitted optical signal is sent to an optical demultiplexer 7 which has the same configuration as the optical combiner 5 but has only the input and output terminals connected in reverse.
is input. Since this optical input signal is intensity-modulated by semiconductor lasers having different oscillation wavelengths, it is demultiplexed by the optical demultiplexer 7 and optical-to-electrical conversion is performed by the respective light receiving elements 9. The optical signal transmitted up to this point is twice or three times the total fundamental wave due to the nonlinearity of the current vs. optical output characteristic of the semiconductor laser.
2nd and 3rd order beat distortion occurs, deteriorating the quality of the signal. The harmonic distortion of the distorted electric signal converted by the light receiving element is removed by the mixer 10 which is constituted by a band pass wave generator. Here, the mixer 10 is set to the center frequency of the carrier wave similarly to the branching filter 2. Then, an electrical signal of only the fundamental wave is obtained at the terminal 11, respectively. In this way, the harmonic components generated by the light emitting elements and the like are removed by the electrical system, so the structure can be very simple.
次に上記発明をシステムに使用した例を示す。
例えば、VHF帯のテレビ信号の光多重伝送を行
う場合について説明すると、現在日本のテレビ周
波数配列は第2図のようになつている。この様な
周波数配列の信号を非直線性の素子に与えると関
東チヤネルの場合は、ローバンドのCH1,CH3
の映像キヤリアの和による2次ビートがCH8の
映像キヤリアと1.25MHzのビートを起し、CH1
とCH3の映像キヤリアの2倍がそれぞれCH6と
CH10の映像キヤリアと0.75MHz、0.25MHzのビ
ートを起す。このビート妨害は、テレビ画面上で
縞模様となり非常に不愉快な妨害となる。本実施
例の装置を第3図に示すと、まずアンテナ20か
ら入つたテレビ信号は、分波器21によりローバ
ンド、ハイバンドに分波されて、それぞれ個別の
増幅器22,23により半導体レーザを駆動でき
るまで増幅される。そしてそれぞれ発振スペクト
ル波長の異なる半導体レーザ24,25にローバ
ンド、ハイバンドに分波されたテレビ信号が加え
られ強度変調される。それぞれ発振スペクトル波
長により強度変調された光出力信号は、半導体レ
ーザ24,25に結合されたフアイバ26,27
に入力され光合成器28に入り、混合され、伝送
用フアイバ29を用いて伝送される。そして光受
信装置において、伝送されてきた光信号は光分波
器30によりローバンド信号とハイバンド信号に
分波されそれぞれフアイバ31,32に出力され
る。それぞれのフアイバ31,32に結合された
受光素子33,34により高調波歪成分を含む光
信号は光―電気変換され、それぞれの増幅器3
5,36により増幅されローバンド、ハイバンド
の波器37により高調波歪成分が除去され、混
合される。そして基本波成分のみテレビ38に入
力される。 Next, an example will be shown in which the above invention is used in a system.
For example, to explain the case of optical multiplex transmission of VHF band television signals, the current television frequency arrangement in Japan is as shown in Figure 2. When a signal with such a frequency arrangement is applied to a non-linear element, in the case of the Kanto channel, low band CH1 and CH3
The secondary beat due to the sum of the video carriers causes a beat of 1.25MHz with the video carrier of CH8, and
and twice the video carrier of CH3 are CH6 and CH3, respectively.
It generates a beat of 0.75MHz and 0.25MHz with the video carrier of CH10. This beat disturbance becomes a striped pattern on the television screen, which is very unpleasant. The apparatus of this embodiment is shown in FIG. 3. First, a television signal input from an antenna 20 is split into a low band and a high band by a splitter 21, and a semiconductor laser is driven by separate amplifiers 22 and 23, respectively. Amplified until possible. Then, the television signal split into low band and high band is applied to the semiconductor lasers 24 and 25, each having a different oscillation spectrum wavelength, and is intensity-modulated. The optical output signals whose intensity is modulated by the oscillation spectrum wavelength are transmitted through fibers 26 and 27 coupled to semiconductor lasers 24 and 25, respectively.
The signals are input to the optical combiner 28, mixed, and transmitted using the transmission fiber 29. In the optical receiver, the transmitted optical signal is demultiplexed into a low band signal and a high band signal by an optical demultiplexer 30, and outputted to fibers 31 and 32, respectively. Optical signals containing harmonic distortion components are optical-to-electrically converted by the light receiving elements 33 and 34 coupled to the respective fibers 31 and 32, and then sent to the respective amplifiers 3.
5 and 36, harmonic distortion components are removed and mixed by a low-band and high-band wave generator 37. Then, only the fundamental wave component is input to the television 38.
第4図には、第3図に示したシステムの各所に
対応したスペクトル波形を示す。図中上段に示し
たスペクトル波形において、40はアンテナ20
で受信したテレビ信号、41は21により分波さ
れたローバンド信号、42はハイバンド信号、4
3は半導体レーザ24,25の電流対光出力特性
の非直線性により歪み、光合成器28により混合
された伝送信号、44は光分波器30により分波
されたローバンド、45はハイバンド信号、46
は波器37により混合されたテレビ信号波形で
ある。上記の実施例では、半導体レーザの電流対
光出力特性の非直線性により生じた歪みを波器
37を通すことによつて除去し、ハイバンド、ロ
ーバンド信号とも基本成分のみを再成できる。従
つて半導体レーザの非直線性とは無関係にテレビ
信号の光多重伝送が可能となる。 FIG. 4 shows spectral waveforms corresponding to various parts of the system shown in FIG. 3. In the spectrum waveform shown in the upper part of the figure, 40 is the antenna 20
41 is the low band signal branched by 21, 42 is the high band signal, 4
3 is a transmission signal distorted by the non-linearity of the current vs. light output characteristics of the semiconductor lasers 24 and 25 and mixed by the optical combiner 28; 44 is a low band signal demultiplexed by an optical demultiplexer 30; 45 is a high band signal; 46
is the television signal waveform mixed by the waver 37. In the above embodiment, the distortion caused by the non-linearity of the current versus optical output characteristic of the semiconductor laser is removed by passing the signal through the wave generator 37, and only the fundamental components of both the high band and low band signals can be regenerated. Therefore, optical multiplex transmission of television signals becomes possible regardless of the nonlinearity of the semiconductor laser.
以上のように本発明によれば、光多重伝送にあ
たつて半導体レーザの非直線動作特性による歪に
対し、個々の半導体レーザの特性とは無関係に元
の信号を再生することが可能であるため、簡素な
構成により光多重伝送を実現できる優れた光多重
伝送方式を提供することができる。 As described above, according to the present invention, it is possible to regenerate the original signal regardless of the characteristics of each individual semiconductor laser in response to distortion caused by the nonlinear operating characteristics of the semiconductor laser during optical multiplex transmission. Therefore, it is possible to provide an excellent optical multiplex transmission system that can realize optical multiplex transmission with a simple configuration.
第1図は本発明の光多重伝送方式を実現するた
めの基本的な構成図、第2図はテレビジヨン信号
の周波数配列図、第3図はテレビ信号を伝送する
一実施例を示す構成図、第4図は第3図に対応さ
せて示した要部伝送スペクトル図である。
1……端子、2……分波器、3……半導体レー
ザ、4……フアイバ、5……光合成器、6……伝
送フアイバ、7……光分波器、8……フアイバ、
9……受光素子、10……混合器。
Fig. 1 is a basic configuration diagram for realizing the optical multiplex transmission system of the present invention, Fig. 2 is a frequency arrangement diagram of a television signal, and Fig. 3 is a configuration diagram showing an embodiment for transmitting a television signal. , FIG. 4 is a transmission spectrum diagram of the main part shown corresponding to FIG. 3. 1...Terminal, 2...Demultiplexer, 3...Semiconductor laser, 4...Fiber, 5...Optical combiner, 6...Transmission fiber, 7...Optical demultiplexer, 8...Fiber,
9... Light receiving element, 10... Mixer.
Claims (1)
力させ、分波された各出力をそれぞれ発光スペク
トル波長の異なる複数個の発光素子により光出力
となし、前記複数の光出力を光学的に合成して伝
送手段に導びき、伝送手段の他方で光分波器に入
力させて分波された光出力となし、この光出力を
前記発光素子と同数の受光素子を開して電気出力
として取り出し、この電気出力を対応する複数個
の帯域通過波器を通過させた後混合して前記般
送波信号を得ることを特徴とする光多重伝送方
式。1. A frequency-multiplexed carrier signal is input to a demultiplexing means, each demultiplexed output is made into an optical output by a plurality of light emitting elements having different emission spectrum wavelengths, and the plurality of optical outputs are optically combined. and guide it to a transmission means, input it to an optical demultiplexer on the other side of the transmission means to produce a demultiplexed optical output, and extract this optical output as an electrical output by opening the same number of light receiving elements as the light emitting elements, An optical multiplex transmission system characterized in that the electrical output is passed through a plurality of corresponding band-pass transducers and then mixed to obtain the general transmission signal.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP120379A JPS5593338A (en) | 1979-01-09 | 1979-01-09 | Optical multiplex transmission system |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP120379A JPS5593338A (en) | 1979-01-09 | 1979-01-09 | Optical multiplex transmission system |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5593338A JPS5593338A (en) | 1980-07-15 |
| JPS6139775B2 true JPS6139775B2 (en) | 1986-09-05 |
Family
ID=11494896
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP120379A Granted JPS5593338A (en) | 1979-01-09 | 1979-01-09 | Optical multiplex transmission system |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5593338A (en) |
Families Citing this family (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4393518A (en) * | 1981-01-16 | 1983-07-12 | Bell Telephone Laboratories, Incorporated | Optical communication arrangement |
| JPH0346842A (en) * | 1989-07-14 | 1991-02-28 | Nec Corp | Fdm optical transmitter |
| US5710653A (en) * | 1995-03-06 | 1998-01-20 | Fiber Optic Network Solutions Corp. | Linear multi-output optical transmitter system |
| JPH0983435A (en) * | 1995-09-20 | 1997-03-28 | Nec Corp | Optical transmitter |
| WO1997049248A1 (en) * | 1996-06-21 | 1997-12-24 | Fiber Optic Network Systems Corp. | Wavelength division multiplexing system |
-
1979
- 1979-01-09 JP JP120379A patent/JPS5593338A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5593338A (en) | 1980-07-15 |
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