JPH1093534A - Optical transmission method - Google Patents

Optical transmission method

Info

Publication number
JPH1093534A
JPH1093534A JP8244643A JP24464396A JPH1093534A JP H1093534 A JPH1093534 A JP H1093534A JP 8244643 A JP8244643 A JP 8244643A JP 24464396 A JP24464396 A JP 24464396A JP H1093534 A JPH1093534 A JP H1093534A
Authority
JP
Japan
Prior art keywords
optical
signal
transmission
wavelength
frequency
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
JP8244643A
Other languages
Japanese (ja)
Inventor
Hideyuki Nasu
秀行 那須
Hideyuki Omura
英之 大村
Nozomi Matsuo
望 松尾
Yukihisa Shinoda
雪久 篠田
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.)
Furukawa Electric Co Ltd
Tokyo Electric Power Company Holdings Inc
Original Assignee
Furukawa Electric Co Ltd
Tokyo Electric Power Co Inc
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 Furukawa Electric Co Ltd, Tokyo Electric Power Co Inc filed Critical Furukawa Electric Co Ltd
Priority to JP8244643A priority Critical patent/JPH1093534A/en
Publication of JPH1093534A publication Critical patent/JPH1093534A/en
Pending legal-status Critical Current

Links

Abstract

PROBLEM TO BE SOLVED: To provide the optical transmission method in which the multiplicity of optical signals arranged in a transmission wavelength band is increased and the number of stations sending a transmission signal is increased by relaxing or eliminating a spread of a beat signal due to chirping toward a frequency direction so as to make a signal wavelength interval narrow. SOLUTION: In this method, two optical signals whose wavelength differs obtained by modulating a light from a light source 1 with an external modulator 3 are sent through one optical transmission line 5 and the two optical signal waves or over are received by a light receiving device 6. The two optical signal waves or over take a wavelength interval where a center frequency of the beat signal generated depending on the wavelength difference is selected to be a multiple of four of a maximum frequency in the transmission band.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明は波長の異なる光信号
を一本の光伝送路により多重伝送する光伝送方法に関す
るものであり、例えば多地点の端局から映像、データ等
の情報を異なる波長の光信号にして一本の光伝送路によ
り中央局に伝送し、多地点の監視、管理を行う場合に利
用される光伝送方法に関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an optical transmission method for multiplexing and transmitting optical signals having different wavelengths through a single optical transmission line. The present invention relates to an optical transmission method which is used when a single optical transmission line is transmitted to a central office through a single optical transmission line to monitor and manage multipoints.

【0002】[0002]

【従来の技術】一本の光ファイバからなる光伝送路によ
り複数の光信号を伝送する方法として図5に示す光伝送
方法が知られている。図5の光伝送方法は、各端局の変
調器11からの信号を光源12(E/O変換器:例えば
LD)により直接変調して、変調して出力された光を光
カプラ13で合波して一本の光ファイバ14に送り込ん
で中央局に多重化された光信号を伝送する。多重化され
た光信号を中央局の受光器15で受光して検波してか
ら、2信号以上に分配し復調器16によりデータ及び映
像信号として復調するものである。図5において、符号
17はテレビモニタである。
2. Description of the Related Art An optical transmission method shown in FIG. 5 is known as a method for transmitting a plurality of optical signals through an optical transmission line comprising one optical fiber. In the optical transmission method of FIG. 5, the signal from the modulator 11 of each terminal is directly modulated by the light source 12 (E / O converter: LD, for example), and the modulated light is combined by the optical coupler 13. The multiplexed optical signal is transmitted to one optical fiber 14 and transmitted to the central office. The multiplexed optical signal is received by the optical receiver 15 of the central office, detected, distributed to two or more signals, and demodulated by the demodulator 16 as data and video signals. In FIG. 5, reference numeral 17 denotes a television monitor.

【0003】ところで、波長の異なる複数の信号伝送で
は受光器において波長の異なる2波以上の光信号の相互
干渉によりビート信号が発生する。ビート信号の発生周
波数帯域は一本の光ファイバで伝送される2波以上の光
信号の波長差に対応する。例えば、図6(a)のように
λ0 、λ1 の2波の光を伝送する場合に無変調である
と、図6(b)に示すようにビート信号が現れる。ここ
で、E/O変換器に変調信号を入力すると図6(c)に
示すようにビート信号が周波数方向に広がるチャーピン
グが発生する。したがって、上述のビート信号が伝送信
号と同一周波数帯域に発生すると、伝送信号の品質は著
しく劣化する。ビート信号による伝送信号の劣化を防ぐ
ためには波長間隔を十分に離す必要がある。同時に、光
源の波長を一定に制御する技術が必要となる。
In the transmission of a plurality of signals having different wavelengths, a beat signal is generated in the optical receiver due to mutual interference between two or more optical signals having different wavelengths. The frequency band in which the beat signal is generated corresponds to the wavelength difference between two or more optical signals transmitted through one optical fiber. For example, when two waves of λ 0 and λ 1 are transmitted as shown in FIG. 6A and no modulation is performed, a beat signal appears as shown in FIG. 6B. Here, when the modulation signal is input to the E / O converter, chirping occurs in which the beat signal spreads in the frequency direction as shown in FIG. Therefore, when the above-mentioned beat signal is generated in the same frequency band as the transmission signal, the quality of the transmission signal is significantly deteriorated. In order to prevent the transmission signal from deteriorating due to the beat signal, it is necessary to sufficiently separate the wavelength intervals. At the same time, a technique for controlling the wavelength of the light source to be constant is required.

【0004】[0004]

【発明が解決しようとする課題】E/O変換器を直接変
調する方法においては、光源、例えばDFBレーザの振
動数が周波数方向に振動する現象(チャーピング)があ
る。また光信号を直接変調する方法で変調するとビート
信号が周波数方向に広がるため、伝送信号がビート信号
と同一周波数帯域にある場合に伝送信号の劣化が生じ
る。すなわち、図6(b)に示すように光源を直接変調
しない場合のビート信号と比較して、図6(c)のよう
に直接変調を行う場合はチャーピングによりビート信号
の周波数帯域が広がる。このために波長間隔の規定を行
うに際して光源の特性であるビート信号のチャーピング
が影響し、波長間隔を狭めることを制限する。光伝送に
用いられる波長資源は有限であるため、伝送局数を増加
することを制限していた。
In a method of directly modulating an E / O converter, there is a phenomenon (chirping) in which the frequency of a light source, for example, a DFB laser vibrates in the frequency direction. When the optical signal is modulated by a direct modulation method, the beat signal spreads in the frequency direction, so that when the transmission signal is in the same frequency band as the beat signal, the transmission signal deteriorates. That is, when the direct modulation is performed as shown in FIG. 6C, the frequency band of the beat signal is expanded by chirping, as compared with the beat signal when the light source is not directly modulated as shown in FIG. 6B. For this reason, when defining the wavelength interval, the chirping of the beat signal, which is a characteristic of the light source, has an effect, and the narrowing of the wavelength interval is restricted. Since the wavelength resources used for optical transmission are finite, increasing the number of transmission stations has been limited.

【0005】本発明は上記の課題を解決し、チャーピン
グによるビート信号の周波数方向への広がりを緩和ある
いはなくし、信号の波長間隔を狭めることにより伝送波
長帯域に配列可能な光信号の多重数を増やし、伝送信号
を発信する局数を増加できる光伝送方法を提供すること
を目的とするものである。
SUMMARY OF THE INVENTION The present invention solves the above-mentioned problem, and reduces or eliminates the spread of a beat signal in the frequency direction due to chirping, and narrows the wavelength interval of the signal to reduce the number of multiplexed optical signals that can be arranged in the transmission wavelength band. It is an object of the present invention to provide an optical transmission method capable of increasing the number of stations transmitting transmission signals.

【0006】[0006]

【課題を解決するための手段】本発明は上記の課題を解
決するために以下のような手段を有している。
The present invention has the following means to solve the above problems.

【0007】本発明の請求項1の光伝送方法は、光源か
らの光を外部変調器により変調した波長の異なる2波以
上の光信号を一本の光伝送路により伝送して前記2波以
上の光信号を受光器で受光する光伝送方法であって、前
記2波以上の光信号はその波長差に応じて発生するビー
ト信号の中心周波数が伝送帯域の最大周波数の4倍以上
となる波長間隔となっていることを特徴とする。
According to a first aspect of the present invention, there is provided an optical transmission method comprising: transmitting two or more optical signals having different wavelengths obtained by modulating light from a light source by an external modulator through a single optical transmission line; An optical transmission method for receiving an optical signal at a photodetector, wherein the two or more optical signals have a wavelength at which the center frequency of a beat signal generated according to the wavelength difference is at least four times the maximum frequency of the transmission band. It is characterized by an interval.

【0008】本発明の請求項2の光伝送方法は、外部変
調器はマッハツェンダー干渉を利用した変調器であるこ
とを特徴とする。
The optical transmission method according to a second aspect of the present invention is characterized in that the external modulator is a modulator utilizing Mach-Zehnder interference.

【0009】本発明の光伝送方法によれば、2波以上の
光信号は外部変調器により変調し、その波長差に応じて
発生するビート信号の中心周波数が伝送帯域の最大周波
数の4倍以上の波長間隔となっているので、チャーピン
グによるビート信号の周波数方向への広がりを緩和ある
いはなくし、信号の波長間隔を狭めることにより伝送波
長帯域に配列可能な光信号の多重数を増やし、伝送信号
を発信する局数を増加することが可能となる。
According to the optical transmission method of the present invention, the optical signal of two or more waves is modulated by the external modulator, and the center frequency of the beat signal generated according to the wavelength difference is at least four times the maximum frequency of the transmission band. Since the wavelength spacing of the signal is reduced or eliminated, the spread of the beat signal in the frequency direction due to chirping is reduced, and the multiplexing number of optical signals that can be arranged in the transmission wavelength band is increased by reducing the wavelength spacing of the signal. Can be increased.

【0010】すなわち、ビート信号は2波以上の光信号
(波長λ0 、波長λ1 )の波長差に応じて発生する。発
生するビート信号の周波数は次式によって示す論理によ
って決定される。 E0 (t)=A0 sin (ω0 t) 受光器で検出され
る波長λ0 のパワー E1 (t)=A1 sin (ω1 t) 受光器で検出され
る波長λ1 のパワー 前記両式により {E0 (t)+E1 (t)}2 =A0 2 sin 2 (ω
0 t)+A1 2 sin 2 (ω 1 t)+A0 1 {cos (ω
0 −ω1 )t−cos (ω0 +ω1 )} E:光の電界、A:定数、ω:光の波長、t:時間 となり、両波長の差分(ω0 −ω1 )が図6(b)のよ
うにビート信号となって現れる。
That is, the beat signal is an optical signal of two or more waves.
(Wavelength λ0, Wavelength λ1) Is generated according to the wavelength difference. Departure
The frequency of the generated beat signal is based on the logic expressed by the following equation.
Is determined. E0(T) = A0sin (ω0t) Detected by the receiver
Wavelength λ0Power E1(T) = A1sin (ω1t) Detected by the receiver
Wavelength λ1The power of に よ り E0(T) + E1(T)}Two= A0 TwosinTwo
0t) + A1 TwosinTwo 1t) + A0A1{Cos (ω
0−ω1) T-cos (ω0+ Ω1)} E: electric field of light, A: constant, ω: wavelength of light, t: time, and the difference between both wavelengths (ω0−ω1) Is in Fig. 6 (b)
It appears as a beat signal.

【0011】例えば、光伝送帯域の光信号λが1.55
μm帯のとき光の波長差1nmにおいて125GHzを
中心周波数にビート信号が発生する。このとき両波長の
和分(ω0 +ω1 )もビート信号となるがその発生周波
数は1014GHzと高く、光伝送帯域から外れるため問
題にならない。E/O変換器を直接変調する従来の方法
では、図7に示すようにチャーピングによりビート信号
が周波数方向に広がるため、伝送帯域の最大周波数が劣
化しない位置に波長間隔を規定する必要があった。これ
に対し、本発明の光伝送方法による外部変調器による変
調では、図7のような周波数方向の広がりはみられない
が、伝送周波数の基本波に対応したピーク、2次高調波
に対応したピーク、3次高調波に対応したピークが発生
する。しかし、これ以上高次の周波数に対応したピーク
は現れず、伝送帯域の最大周波数がビート信号の3次高
調波に対応したピークよりビート中心周波数に近づかな
いように波長間隔を規定すればよい。
For example, if the optical signal λ in the optical transmission band is 1.55
In the μm band, a beat signal is generated with a center frequency of 125 GHz at a wavelength difference of light of 1 nm. At this time, the sum of the two wavelengths (ω 0 + ω 1 ) also becomes a beat signal, but its generation frequency is as high as 10 14 GHz, which is out of the optical transmission band, and poses no problem. In the conventional method of directly modulating the E / O converter, the beat signal spreads in the frequency direction due to chirping as shown in FIG. 7, so that it is necessary to define the wavelength interval at a position where the maximum frequency of the transmission band does not deteriorate. Was. On the other hand, in the modulation by the external modulator according to the optical transmission method of the present invention, the spread in the frequency direction as shown in FIG. 7 is not observed, but the peak corresponding to the fundamental wave of the transmission frequency and the second harmonic are supported. Peaks and peaks corresponding to the third harmonic are generated. However, a wavelength interval may be defined so that no peak corresponding to a higher-order frequency appears any more, and the maximum frequency of the transmission band does not approach the beat center frequency more than the peak corresponding to the third harmonic of the beat signal.

【0012】例えば、具体的には外部変調器による伝送
帯域は3GHz程度であり、90%程度の変調度を前提
にすると、外部変調による伝送方法では伝送帯域の最大
周波数3GHzとビート信号の3次高調波に対応したピ
ークが同一周波数とならず、かつビート信号の中心周波
数方向に入り込まない波長間隔としては、ビート信号の
中心周波数が伝送帯域の最大周波数3GHzの4倍、す
なわち12GHz以上となり、波長間隔は0.1nm以
上となる。伝送帯域の最大周波数が低周波数で、例えば
ビート信号の中心周波数から4GHz離れた周波数に所
要品質の境界がある場合、伝送帯域の最大周波数はビー
ト信号の中心周波数から4GHz以上離して配置する必
要がある。今、伝送帯域の最大周波数が1GHzの場合
には、所要品質を満足して伝送するには、ビート信号の
中心周波数は5GHz以上となり、2波以上の波長間隔
が0.04nm以上となる。
For example, specifically, the transmission band of the external modulator is about 3 GHz, and assuming a modulation degree of about 90%, the maximum frequency of the transmission band of 3 GHz and the third order of the beat signal are obtained in the transmission method by the external modulation. As a wavelength interval at which the peak corresponding to the harmonic does not become the same frequency and does not enter the direction of the center frequency of the beat signal, the center frequency of the beat signal is four times the maximum frequency 3 GHz of the transmission band, that is, 12 GHz or more. The interval is 0.1 nm or more. When the maximum frequency of the transmission band is a low frequency, for example, when there is a boundary of required quality at a frequency 4 GHz away from the center frequency of the beat signal, the maximum frequency of the transmission band needs to be arranged at least 4 GHz away from the center frequency of the beat signal. is there. Now, if the maximum frequency of the transmission band is 1 GHz, the center frequency of the beat signal is 5 GHz or more and the wavelength interval of two or more waves is 0.04 nm or more in order to transmit the signal with required quality.

【0013】通常用いられる光伝送用の光源であるDF
Bレーザの波長可変幅は温度で規定され1℃で0.1n
m変化し、温度可変幅は通常±5℃であるから波長可変
実力は1nmである。ここで伝送端局数を10端局と
し、等間隔で波長を配列すると波長間隔は0.1nm以
下となる。すなわち、波長間隔を0.04nm以上0.
1nm以下に規定すれば伝送品質を劣化させず伝送可能
となる。以上説明したように、外部変調器を用いるとチ
ャーピングが原理的になくなり、波長間隔を狭められ、
光源の波長選別を行う必要性がなくなる。
DF which is a light source for light transmission which is usually used
The wavelength variable width of the B laser is specified by the temperature and is 0.1 n at 1 ° C.
m, and the temperature variable width is usually ± 5 ° C., so that the actual wavelength variable ability is 1 nm. Here, when the number of transmission terminal stations is set to ten and the wavelengths are arranged at equal intervals, the wavelength interval becomes 0.1 nm or less. That is, the wavelength interval is set to 0.04 nm or more.
If the thickness is set to 1 nm or less, transmission becomes possible without deteriorating the transmission quality. As described above, when an external modulator is used, chirping is basically eliminated, the wavelength interval is narrowed,
There is no need to perform wavelength selection of the light source.

【0014】[0014]

【発明の実施の形態】以下に本発明に係る光伝送方法を
実施の形態により図1ないし図4を参照してより詳細に
説明する。図1(a)、(b)、(c)は本発明の光伝
送方法の実施の形態を示す説明図で、複数の端局の光源
1(E/O変換器:例えばDFBレーザ)から出力した
光を外部変調信号源2からの伝送信号により、例えばマ
ッハツェンダー干渉を利用した変調器からなる外部変調
器3を駆動してその光信号を強度変調し、この強度変調
された光信号を光カプラ4で合波して一本の光伝送路
(光ファイバ)5に送り込んで中央局に多重化された光
信号を伝送する。多重化された光信号を中央局の受光器
6で受光して検波してから、2信号以上に分配し復調器
7によりデータ及び映像信号として復調して、例えばモ
ニタテレビ8で受像するものである。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS Hereinafter, an optical transmission method according to the present invention will be described in more detail with reference to FIGS. FIGS. 1A, 1B, and 1C are explanatory views showing an embodiment of an optical transmission method according to the present invention, wherein outputs from light sources 1 (E / O converters: for example, DFB lasers) of a plurality of terminal stations are provided. The modulated light is driven by a transmission signal from the external modulation signal source 2 to drive, for example, an external modulator 3 including a modulator utilizing Mach-Zehnder interference, and the optical signal is intensity-modulated. The optical signals are multiplexed by the coupler 4 and sent to one optical transmission line (optical fiber) 5 to transmit the multiplexed optical signal to the central office. The multiplexed optical signal is received and detected by the optical receiver 6 of the central office, then distributed into two or more signals, demodulated by the demodulator 7 as data and video signals, and received by, for example, the monitor television 8. is there.

【0015】図1(a)はバス型、(b)はスター型、
(c)はバススター型のシステム形態を示すもので、本
発明の光伝送方法はいずれのシステム形態にでも適応で
きるものである。図1に示す光伝送方法の各システム形
態において、受光器6で検波する際に、光伝送路5によ
り伝送される波長の異なる2以上の光の波長差成分に相
当する周波数に光の相互干渉によるビート信号が発生す
る。ビート信号が変調器3から送出される変調信号の周
波数帯域に発生すると伝送品質が著しく劣化する。ビー
ト信号の発生周波数は光伝送路5に多重される光信号の
波長差に対応して決まり、1nmの波長間隔に対してビ
ート信号の中心周波数は125GHzの位置に発生す
る。
1A is a bus type, FIG. 1B is a star type,
(C) shows a bus star type system configuration, and the optical transmission method of the present invention can be applied to any system configuration. In each system configuration of the optical transmission method shown in FIG. A beat signal is generated. If a beat signal is generated in the frequency band of the modulated signal sent from the modulator 3, the transmission quality is significantly deteriorated. The frequency at which the beat signal is generated is determined according to the wavelength difference of the optical signal multiplexed on the optical transmission line 5, and the center frequency of the beat signal is generated at a position of 125 GHz for a wavelength interval of 1 nm.

【0016】上述のように、外部変調によって光を変調
すると図2で示すように、基本波、2次高調波、3次高
調波に対応したピークが現れる。このとき、伝送信号の
最大周波数がビート信号の3次高調波に対応したピーク
と同一周波数になると伝送品質は劣化する。また、図3
に示すように、変調度90%までの範囲で、ビート信号
にはビート中心周波数及び伝送信号の基本波、2次高調
波、3次高調波に対応するピークが現れる。このピーク
における相対強度雑音は著しく劣化する。従って、伝送
信号の最大周波数がビート信号の中心周波数からビート
信号の3次高調波に対応するピークより、離れた位置に
なるようにすることによって伝送品質は劣化せず伝送で
きる。
As described above, when light is modulated by external modulation, peaks corresponding to the fundamental wave, the second harmonic, and the third harmonic appear as shown in FIG. At this time, if the maximum frequency of the transmission signal becomes the same frequency as the peak corresponding to the third harmonic of the beat signal, the transmission quality deteriorates. FIG.
As shown in the figure, the beat signal has peaks corresponding to the beat center frequency and the fundamental wave, the second harmonic, and the third harmonic of the transmission signal in the range up to the modulation factor of 90%. The relative intensity noise at this peak is significantly degraded. Therefore, by setting the maximum frequency of the transmission signal at a position farther from the center frequency of the beat signal than the peak corresponding to the third harmonic of the beat signal, transmission can be performed without deteriorating the transmission quality.

【0017】本発明の光伝送方法は、波長間隔をビート
信号の中心周波数に対して伝送帯域の最大周波数の4倍
以上になるように規定する。例えば、伝送帯域の最大周
波数が3GHzの場合、ビート信号の中心周波数は12
GHz以上に規定し、このとき波長間隔は0.1nm以
上とする。図1に示す各システム形態において、図4に
示すようにビート信号の中心周波数から4GHz離れた
周波数に所要品質の境界がある場合は伝送帯域の最大周
波数をビート信号の中心周波数から4GHz以上離して
配置する。この場合、所要品質を満足して伝送するに
は、例えば、伝送帯域の最大周波数が1GHzとする
と、ビートの中心周波数は5GHz以上にする必要があ
る。1.55μm帯の光源においては波長間隔1nmで
ビート中心周波数が125GHzであるから、2波以上
の波長間隔を0.04nm以上に規定する。
In the optical transmission method of the present invention, the wavelength interval is defined so as to be at least four times the maximum frequency of the transmission band with respect to the center frequency of the beat signal. For example, if the maximum frequency of the transmission band is 3 GHz, the center frequency of the beat signal is 12
GHz or more, and at this time, the wavelength interval is 0.1 nm or more. In each system configuration shown in FIG. 1, when there is a boundary of required quality at a frequency 4 GHz away from the center frequency of the beat signal as shown in FIG. 4, the maximum frequency of the transmission band is separated from the center frequency of the beat signal by 4 GHz or more. Deploy. In this case, in order to satisfy the required quality and transmit, for example, if the maximum frequency of the transmission band is 1 GHz, the center frequency of the beat needs to be 5 GHz or more. In a 1.55 μm band light source, the wavelength interval is 1 nm and the beat center frequency is 125 GHz. Therefore, the wavelength interval of two or more waves is specified to be 0.04 nm or more.

【0018】以上のようにマッハツェンダー干渉を利用
した変調器からなる外部変調器を用いるとチャーピング
が原理的になくなり、波長間隔を狭められ、光源の波長
選別を行う必要性はなくなる。通常用いられる光伝送用
の光源であるDFBレーザの波長可変幅は温度で規定さ
れ1℃で0.1nm変化し、温度可変幅は通常±5℃で
あるから波長可変実力は1nmである故、伝送端局数を
10端局とし、等間隔で波長を配列すると波長間隔は
0.1nm以下となる。
As described above, when an external modulator including a modulator utilizing Mach-Zehnder interference is used, chirping is eliminated in principle, the wavelength interval is narrowed, and the necessity of wavelength selection of a light source is eliminated. The wavelength tunable width of a DFB laser, which is a light source for optical transmission that is usually used, is defined by temperature and changes by 0.1 nm at 1 ° C. Since the temperature tunable width is usually ± 5 ° C., the actual wavelength tunable is 1 nm If the number of transmission terminal stations is 10 and the wavelengths are arranged at equal intervals, the wavelength interval is 0.1 nm or less.

【0019】以上説明したように、ビート信号には、ビ
ート信号のピーク以外に伝送信号の雑音特性から規定さ
れる所要品質の境界がビート信号の中心周波数から4G
Hzに存在する。したがって、伝送信号はビート信号の
中心周波数から4GHz以上離れた周波数でなければ所
要品質を満たさない。ビート信号のピークによる所要品
質の境界と雑音特性による所要品質の境界が重なるのは
1.33GHzであり、この周波数以下ではビート信号
の雑音特性の境界によって伝送信号の所要品質を満たす
波長間隔を規定する必要があり、1.33GHz以下の
周波数にあっては、波長間隔は0.4nm以上に規定す
ることで伝送が可能となる。
As described above, in the beat signal, in addition to the peak of the beat signal, the boundary of required quality defined by the noise characteristics of the transmission signal is 4G from the center frequency of the beat signal.
Hz. Therefore, the required quality of the transmission signal is not satisfied unless the frequency is at least 4 GHz away from the center frequency of the beat signal. The boundary of the required quality due to the peak of the beat signal and the boundary of the required quality due to the noise characteristic overlap at 1.33 GHz. Below this frequency, the wavelength interval satisfying the required quality of the transmission signal is defined by the boundary of the noise characteristic of the beat signal. In the case of a frequency of 1.33 GHz or less, transmission becomes possible by setting the wavelength interval to 0.4 nm or more.

【0020】なお、上記の実施の形態において、外部変
調器はマッハツェンダー干渉を利用した変調器を使用し
た場合について説明したが、変調器はマッハツェンダー
干渉を利用した変調器に限るものではなくマッハツェン
ダー干渉を利用した変調器以外の他の種類の外部変調器
である電界吸収型変調器等、マッハツェンダー干渉を利
用した変調器以外の周知の外部変調器も使用できる。ま
た、上記の実施の形態において、伝送信号は映像につい
て説明したが、伝送信号は映像以外にもデータ、音声等
の伝送が可能であることはいうまでもない。
In the above embodiment, a case has been described where an external modulator uses a modulator utilizing Mach-Zehnder interference. However, the modulator is not limited to a modulator utilizing Mach-Zehnder interference, and Well-known external modulators other than modulators using Mach-Zehnder interference, such as electroabsorption modulators, which are other types of external modulators other than modulators using Zender interference, can also be used. Further, in the above-described embodiment, the transmission signal has been described for a video, but it goes without saying that the transmission signal can transmit data, audio, and the like in addition to the video.

【0021】[0021]

【発明の効果】以上述べたように、本発明の請求項1の
光伝送方法によれば、2波以上の光信号は外部変調器に
より変調し、その波長差に応じて発生するビート信号の
中心周波数が伝送帯域の最大周波数の4倍以上の波長間
隔となっているので、チャーピングによるビート信号の
周波数方向への広がりを緩和あるいはなくし、信号の波
長間隔を狭めることにより伝送波長帯域に配列可能な光
信号の多重数を増やし、伝送信号を発信する局数を増加
することが可能となる。
As described above, according to the optical transmission method of the first aspect of the present invention, the optical signal of two or more waves is modulated by the external modulator, and the beat signal generated according to the wavelength difference is modulated. Since the center frequency is at least four times the wavelength interval of the maximum frequency of the transmission band, the spread of the beat signal in the frequency direction due to chirping is reduced or eliminated, and the signal wavelength interval is reduced by narrowing the signal wavelength interval. It is possible to increase the number of multiplexable optical signals and increase the number of stations transmitting transmission signals.

【0022】本発明の請求項2の光伝送方法によれば、
原理的にチャーピングのないマッハツェンダー干渉を利
用した変調器を使用することにより、ビート信号が通信
帯域における伝送信号の所要品質を劣化させることなく
がなる。
According to the optical transmission method of the second aspect of the present invention,
The use of a modulator utilizing Mach-Zehnder interference without chirping in principle prevents the beat signal from deteriorating the required quality of the transmission signal in the communication band.

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

【図1】本発明に係る光伝送方法の実施の形態を示す説
明図である。
FIG. 1 is an explanatory diagram showing an embodiment of an optical transmission method according to the present invention.

【図2】外部変調器により変調した場合のビート信号と
伝送帯域の関係を示す説明図である。
FIG. 2 is an explanatory diagram showing a relationship between a beat signal and a transmission band when modulated by an external modulator.

【図3】ビート周波数に対して変化する相対強度雑音の
関係を示す説明図である。
FIG. 3 is an explanatory diagram showing a relationship of a relative intensity noise that changes with respect to a beat frequency.

【図4】ビート信号と所要品質の関係を示す説明図であ
る。
FIG. 4 is an explanatory diagram showing a relationship between a beat signal and required quality.

【図5】従来の光伝送方法の一例を示す説明図である。FIG. 5 is an explanatory diagram showing an example of a conventional optical transmission method.

【図6】従来の光伝送方法における光信号の波長間隔と
ビート信号の関係を示す説明図である。
FIG. 6 is an explanatory diagram showing a relationship between a wavelength interval of an optical signal and a beat signal in a conventional optical transmission method.

【図7】光信号を直接変調した場合のビート信号と伝送
帯域の関係を示す説明図である。
FIG. 7 is an explanatory diagram showing a relationship between a beat signal and a transmission band when an optical signal is directly modulated.

【符号の説明】[Explanation of symbols]

1 光源 2 外部変調信号源 3 外部変調器 4 光カプラ 5 光伝送路 6 受光器 7 復調器 8 モニタテレビ Reference Signs List 1 light source 2 external modulation signal source 3 external modulator 4 optical coupler 5 optical transmission line 6 light receiver 7 demodulator 8 monitor TV

フロントページの続き (72)発明者 松尾 望 東京都千代田区丸の内2丁目6番1号 古 河電気工業株式会社内 (72)発明者 篠田 雪久 東京都千代田区内幸町1丁目1番3号 東 京電力株式会社内Continued on the front page (72) Inventor Nozomu Matsuo 2-6-1 Marunouchi, Chiyoda-ku, Tokyo Inside Furukawa Electric Co., Ltd. (72) Inventor Yukihisa Shinoda 1-3-1 Uchisaiwaicho, Chiyoda-ku, Tokyo Tokyo Inside Electric Power Company

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】 光源からの光を外部変調器により変調し
た波長の異なる2波以上の光信号を一本の光伝送路によ
り伝送して前記2波以上の光信号を受光器で受光する光
伝送方法であって、前記2波以上の光信号はその波長差
に応じて発生するビート信号の中心周波数が伝送帯域の
最大周波数の4倍以上となる波長間隔となっていること
を特徴とする光伝送方法。
1. A light for transmitting two or more optical signals having different wavelengths obtained by modulating light from a light source by an external modulator through one optical transmission line, and receiving the two or more optical signals by a light receiver. A transmission method, wherein the two or more optical signals have a wavelength interval such that the center frequency of the beat signal generated according to the wavelength difference is at least four times the maximum frequency of the transmission band. Optical transmission method.
【請求項2】 外部変調器はマッハツェンダー干渉を利
用した変調器であることを特徴とする請求項1記載の光
伝送方法。
2. The optical transmission method according to claim 1, wherein the external modulator is a modulator using Mach-Zehnder interference.
JP8244643A 1996-09-17 1996-09-17 Optical transmission method Pending JPH1093534A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8244643A JPH1093534A (en) 1996-09-17 1996-09-17 Optical transmission method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8244643A JPH1093534A (en) 1996-09-17 1996-09-17 Optical transmission method

Publications (1)

Publication Number Publication Date
JPH1093534A true JPH1093534A (en) 1998-04-10

Family

ID=17121807

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8244643A Pending JPH1093534A (en) 1996-09-17 1996-09-17 Optical transmission method

Country Status (1)

Country Link
JP (1) JPH1093534A (en)

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