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JPS6235084B2 - - Google Patents
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JPS6235084B2 - - Google Patents

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Publication number
JPS6235084B2
JPS6235084B2 JP56168545A JP16854581A JPS6235084B2 JP S6235084 B2 JPS6235084 B2 JP S6235084B2 JP 56168545 A JP56168545 A JP 56168545A JP 16854581 A JP16854581 A JP 16854581A JP S6235084 B2 JPS6235084 B2 JP S6235084B2
Authority
JP
Japan
Prior art keywords
wavelength
optical
light
circuit
optical fiber
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
Application number
JP56168545A
Other languages
Japanese (ja)
Other versions
JPS5870652A (en
Inventor
Koichi Minemura
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
Nippon Electric Co 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 Nippon Electric Co Ltd filed Critical Nippon Electric Co Ltd
Priority to JP56168545A priority Critical patent/JPS5870652A/en
Publication of JPS5870652A publication Critical patent/JPS5870652A/en
Publication of JPS6235084B2 publication Critical patent/JPS6235084B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04JMULTIPLEX COMMUNICATION
    • H04J14/00Optical multiplex systems
    • H04J14/02Wavelength-division multiplex systems
    • H04J14/03WDM arrangements
    • H04J14/0305WDM arrangements in end terminals

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】 この発明は波長多重光フアイバ伝送システム、
特に光源が半導体レーザで多重されるチヤンネル
数が3以上の場合に適する波長多重光フアイバ伝
送システムに関するものである。
[Detailed Description of the Invention] This invention provides a wavelength multiplexed optical fiber transmission system,
In particular, the present invention relates to a wavelength multiplexing optical fiber transmission system suitable for a case where the light source is a semiconductor laser and the number of multiplexed channels is three or more.

光の波長が異なることを利用して複数の光を多
重し、一本の光フアイバで伝送する波長多重光フ
アイバ伝送技術は、伝送路光フアイバの経済的利
用が可能なこと、既存電気回路の壁を破るような
大容量伝送が可能なこと、たとえばチヤンネルの
増設が伝送路光フアイバに関係なく光送受信機や
光合波分波回路の変更だけで出来るといつたよう
にシステム的柔軟性が高いこと、又アナログ信号
とデジタル信号等の異種信号の多重伝送が可能な
こと等の種々の長所を有しており、近距離低速伝
送系から長距離高速伝送系にいたる種々の伝送系
を対象として最近活発に研究開発されている。
Wavelength multiplexing optical fiber transmission technology, which uses the different wavelengths of light to multiplex multiple lights and transmit them through a single optical fiber, is capable of economical use of transmission line optical fibers and is easy to use in existing electrical circuits. It is possible to transmit large amounts of data that can break through walls, and has high system flexibility; for example, channels can be added by simply changing the optical transmitter/receiver and optical multiplexing/demultiplexing circuit, regardless of the optical fiber used for the transmission route. It also has various advantages such as being able to multiplex transmission of different types of signals such as analog signals and digital signals, and is suitable for various transmission systems ranging from short-distance low-speed transmission systems to long-distance high-speed transmission systems. It has been actively researched and developed recently.

光合波回路(光多重回路とも言われる)や光分
波回路としては誘電体多層膜(干渉膜)の光反
射・透過特性が波長依存性を有することを利用し
た干渉膜型や、回折格子で回折される光の角度が
波長依存性を有することを利用した回折格子型の
回路が一般に用いられることが多い。
For optical multiplexing circuits (also called optical multiplexing circuits) and optical demultiplexing circuits, there are interference film types that take advantage of the wavelength dependence of the light reflection and transmission characteristics of dielectric multilayer films (interference films), and diffraction gratings. Generally, a diffraction grating type circuit is often used, which takes advantage of the fact that the angle of diffracted light has wavelength dependence.

ところで干渉膜型では、干渉膜のきれがよくな
いために波長間隔が狭くできないという欠点と、
チヤンネル数が多い場合には干渉膜型回路を多段
にしなければならないために挿入損失が大きく且
つ構造が複雑になるという欠点とがあり、したが
つてチヤンネル数の実用的な上限は4程度であ
る。
However, the interference film type has the disadvantage that the wavelength interval cannot be narrowed because the interference film is not sharp.
When the number of channels is large, the interference film type circuit must be multi-staged, resulting in a large insertion loss and a complicated structure, so the practical upper limit for the number of channels is about 4. .

一方回折格子型では、チヤンネル数を多くする
ことは干渉膜型よりは容易であるが、光が出射さ
れる側の光フアイバのコア径を光が入射される側
の光フアイバのコア径よりも十分に大きくしない
と、光源の波長変化が生じた場合回折された光が
出射側の光フアイバに入力しなくなり、わずかの
波長変化で挿入損失が大きく増加する等の欠点が
ある。ところが回折格子型の光合波回路では、出
射側の光フアイバとなる伝送路光フアイバのコア
径等は、周波数帯域等の観点からシステム設計で
一義的に定まることが多いために、上記の欠点を
この光合波回路で回避しようとして入射側の光フ
アイバのコア径を十分小さくすると、この回路の
外においてこの光フアイバと光源の間の結合効率
が悪くなるという欠点が生じる。特に伝送路光フ
アイバが単一モード光フアイバの場合には、一般
にコア径が10μm以下なので、回折格子型の光合
波回路は実現困難な状況にある。なお回折格子型
の光分波回路は、出射側の光フアイバから出力さ
れる光は一般に伝送路光フアイバのコア径よりも
大きい受光径を持つ光検出器に導かれるので、出
射側の光フアイバのコア径を大きくすることは容
易で、10チヤンネル以上のものが開発されてい
る。
On the other hand, with the diffraction grating type, it is easier to increase the number of channels than with the interference film type, but the core diameter of the optical fiber on the side where the light is emitted is set to be smaller than the core diameter of the optical fiber on the side where the light enters. If it is not made sufficiently large, the diffracted light will not enter the output side optical fiber when the wavelength of the light source changes, resulting in disadvantages such as a slight change in wavelength will greatly increase insertion loss. However, in diffraction grating type optical multiplexing circuits, the core diameter of the transmission line optical fiber, which is the optical fiber on the output side, is often uniquely determined by system design from the viewpoint of frequency band, etc., so the above drawbacks cannot be overcome. If the core diameter of the optical fiber on the input side is made sufficiently small in order to avoid this problem with this optical multiplexing circuit, a drawback arises in that the coupling efficiency between the optical fiber and the light source deteriorates outside the circuit. In particular, when the transmission line optical fiber is a single mode optical fiber, the core diameter is generally 10 μm or less, making it difficult to realize a diffraction grating type optical multiplexing circuit. In addition, in a diffraction grating type optical demultiplexing circuit, the light output from the optical fiber on the output side is generally guided to a photodetector having a receiving diameter larger than the core diameter of the transmission line optical fiber. It is easy to increase the core diameter, and those with more than 10 channels have been developed.

以上のような観点から、チヤンネル数が4以下
の波長多重光フアイバ伝送システムでは、一般に
光合波回路には干渉膜型が、光分波回路には干渉
膜型または回折格子型が使用されてきている。そ
してチヤンネル数が5以上のシステムでは、光合
波回路としては回折型は全く使用できず、干渉膜
型も回路の挿入損失が大きいためにシステムの許
容伝送路損失が小さくなつて伝送路距離が短かく
ならざるを得ず、而もこのシステムではチヤンネ
ル間の波長間隔が狭く出来ないから広い波長範囲
が必要であり、このために伝送路光フアイバの損
失の大きい波長範囲も使わざるを得ないために、
伝送路距離はさらに短かくなるという欠点があつ
た。
From the above points of view, in wavelength multiplexing optical fiber transmission systems with a channel number of 4 or less, an interference film type is generally used for the optical multiplexing circuit, and an interference film type or a diffraction grating type is used for the optical demultiplexing circuit. There is. In systems with five or more channels, the diffraction type cannot be used at all as an optical multiplexing circuit, and the interference film type also has a large circuit insertion loss, which reduces the system's allowable transmission line loss and shortens the transmission line distance. This is unavoidable, because in this system, the wavelength interval between channels cannot be narrowed, so a wide wavelength range is required, and for this reason, the wavelength range where the transmission line optical fiber has a large loss must also be used. To,
The disadvantage was that the transmission path distance became even shorter.

なお光合波回路に回折格子型を使うことができ
ないのにはもう1つの理由がある。即ちこの場合
には、光源の波長の温度変化により光合波回路の
挿入損失が大きくなるという欠点があつた。その
ために、ある使用温度範囲を考えると、システム
の許容伝送路損失が低くできない、伝送路距離が
長く出来ないという欠点があるからである。特
に、伝送路光フアイバが単一モード光フアイバの
場合には、この欠点は大きく、回折格子型の光合
波回路を使うシステムは不可能であつた。
There is another reason why a diffraction grating type cannot be used in an optical multiplexing circuit. That is, in this case, there was a drawback that the insertion loss of the optical multiplexing circuit increased due to temperature changes in the wavelength of the light source. For this reason, considering a certain operating temperature range, there are disadvantages in that the permissible transmission line loss of the system cannot be lowered and the transmission line distance cannot be increased. This drawback is particularly severe when the transmission line optical fiber is a single mode optical fiber, and a system using a diffraction grating type optical multiplexing circuit is impossible.

したがつて本発明の目的は、チヤンネル数が3
以上の場合に、従来よりも伝送路距離が長く出来
る波長多重光フアイバ伝送システムを提供するこ
とにある。
Therefore, an object of the present invention is to reduce the number of channels to 3.
In the above case, it is an object of the present invention to provide a wavelength division multiplexing optical fiber transmission system that allows the transmission line distance to be longer than the conventional one.

この発明によれば、互いに発振波長の異なる少
なくとも3個の半導体レーザ、これら半導体レー
ザの出力光の波長多重を行う光合波手段、波長多
重された光を伝搬する伝送路光フアイバ、伝播さ
れた光を波長毎に分波する分波回路、および分波
した各波長の光を検出する光検出器を含む光フア
イバ伝送システムにおいて、前記光合波手段が、
前記半導体レーザの出力光を入力とし、少くとも
1つの波長依存性のある光多重回路を含む光多重
手段と、前記少くとも1つの波長依存性のある光
多重回路の出力及び他の波長依存性のある光多重
回路の出力又は前記入力した半導体レーザの出力
光を合成して前記波長多重された光を出力する波
長依存性のない単一の光多重回路とから成り、而
して前記光多重手段の波長依存性のある光多重回
路に割当てられる少なくとも2つのレーザ光の波
長が、その大きさの順に少なくとも1つはなれて
いることを特徴とする波長多重光フアイバ伝送シ
ステムが得られる。
According to the present invention, at least three semiconductor lasers having different oscillation wavelengths, an optical multiplexing means for wavelength-multiplexing the output lights of these semiconductor lasers, a transmission line optical fiber for propagating the wavelength-multiplexed light, and the propagated light In an optical fiber transmission system including a demultiplexing circuit that demultiplexes the light of each wavelength, and a photodetector that detects the demultiplexed light of each wavelength, the optical multiplexing means
an optical multiplexing means that receives the output light of the semiconductor laser as an input and includes at least one wavelength-dependent optical multiplexing circuit; and an output of the at least one wavelength-dependent optical multiplexing circuit and other wavelength-dependent optical multiplexing circuits; The output of an optical multiplexing circuit or a single wavelength-independent optical multiplexing circuit that combines the output lights of the inputted semiconductor lasers and outputs the wavelength-multiplexed light; A wavelength multiplexing optical fiber transmission system is obtained in which the wavelengths of at least two laser beams assigned to the wavelength-dependent optical multiplexing circuit of the means are different in order of magnitude by at least one wavelength.

次に図面を参照して詳細に説明する。 Next, a detailed description will be given with reference to the drawings.

第1図はこの発明の波長多重光フアイバ伝送シ
ステムの最も好ましい実施例の構成を示すブロツ
ク図である。第1〜第6の光送信機1〜6の第1
〜第6の信号入力端子11〜16にそれぞれ入力
された電気信号は、第1〜第6の送信回路21〜
26でそれぞれ増幅等を受け、第1〜第6の半導
体レーザ31〜36にそれぞれ印加されて光信号
に変換される。ここに第1〜第6の半導体レーザ
31〜36の出力光の波長λ,λ,………λ
は850nm、860nm、870nm、880nm、890nm
にそれぞれ設定されている。これら第1〜第6の
半導体レーザ31〜36は活性層がGaAsでこの
活性層の両側にAlXGa1-XAs層を備えたダブルヘ
テロ構造を有しており、主に活性層中に混入させ
る微量なAlの量を制御することにより前記のよ
うな800nm帯の所望の波長の光が出力するよう
にしてある。
FIG. 1 is a block diagram showing the configuration of the most preferred embodiment of the wavelength division multiplexing optical fiber transmission system of the present invention. The first of the first to sixth optical transmitters 1 to 6
The electrical signals input to the ~sixth signal input terminals 11~16 are transmitted to the first~sixth transmitter circuits 21~
26, the signals are amplified, etc., and applied to the first to sixth semiconductor lasers 31 to 36, respectively, and converted into optical signals. Here, the wavelengths λ 1 , λ 2 , ...... λ of the output lights of the first to sixth semiconductor lasers 31 to 36 are
6 is 850nm, 860nm, 870nm, 880nm, 890nm
are set respectively. These first to sixth semiconductor lasers 31 to 36 have a double heterostructure in which the active layer is GaAs and Al x Ga 1-x As layers are provided on both sides of the active layer. By controlling the minute amount of Al mixed in, light of the desired wavelength in the 800 nm band as described above is output.

上記のような第1〜第6の半導体レーザ31〜
36の出力光は第1〜第6の結合回路41〜46
によりそれぞれ集光されて第1〜第6の光フアイ
バ51〜56にそれぞれ結合される。これらの第
1〜第6の光フアイバ51〜56はコア−長軸の
長さが10μm、短軸の長さが7μmの楕円形コア
を有する偏波面保存光フアイバで、これら光フア
イバに直線偏光が入力された場合には同じ偏波面
の直線偏光を出力する特性を有している。
First to sixth semiconductor lasers 31 as described above
The output light of 36 is connected to the first to sixth coupling circuits 41 to 46.
The light is condensed and coupled to the first to sixth optical fibers 51 to 56, respectively. These first to sixth optical fibers 51 to 56 are polarization maintaining optical fibers having an elliptical core with a long axis length of 10 μm and a short axis length of 7 μm. It has a characteristic of outputting linearly polarized light with the same polarization plane when it is input.

上記の第1〜第6の光フアイバのうち、第1、
第3、第5の光フアイバ51,53,55は干渉
型の波長依存性を有する第1の光多重回路201
に接続されており、第1、第3、第5の半導体レ
ーザ31,33,35の出力光の第1図の紙面に
平行な偏波面を有する直線偏光が波長多重されて
第7の光フアイバ57に導かれ、同様に、第2、
第4、第6の光フアイバ52,54,56は同じ
く干渉膜型の波長依存性を有する第2の光多重回
路202に接続されており、第2、第4、第6の
半導体レーザ32,34,36の出力光の第1図
の紙面に垂直な偏波面の直線偏光が波長多重され
て第8の光フアイバ58に導かれる。ここに第7
および第8の光フアイバはいずれも第1〜第6の
光フアイバと同じ特性を持たせてある。
Among the first to sixth optical fibers, the first,
The third and fifth optical fibers 51, 53, and 55 are connected to a first optical multiplex circuit 201 having interference type wavelength dependence.
The output lights of the first, third, and fifth semiconductor lasers 31, 33, and 35 are wavelength-multiplexed and the linearly polarized light having a plane of polarization parallel to the plane of the paper in FIG. 57, similarly, the second,
The fourth and sixth optical fibers 52, 54, and 56 are connected to a second optical multiplexing circuit 202 which also has interference film type wavelength dependence, and the second, fourth, and sixth semiconductor lasers 32, The linearly polarized lights of the output lights 34 and 36 whose plane of polarization is perpendicular to the paper plane of FIG. here number 7
Both of the optical fibers and the eighth optical fiber have the same characteristics as the first to sixth optical fibers.

第7、第8の光フアイバ57と58は、波長依
存性がなく偏波面光多重回路構成を持つ第3の光
多重回路203に接続されており、互に偏波面の
直交する2つの直線偏光は多重されて伝送路光フ
アイバ59に導かれている。伝送路光フアイバ5
9はコア径が50μm、フアイバ外径が125μm、
開口数(N.A.)が0.2の集束型マルチモード光フ
アイバで出来ている。
The seventh and eighth optical fibers 57 and 58 are connected to a third optical multiplexing circuit 203 that has no wavelength dependence and has a polarization plane optical multiplexing circuit configuration, and are connected to two linearly polarized lights whose polarization planes are orthogonal to each other. are multiplexed and guided to a transmission path optical fiber 59. Transmission line optical fiber 5
9 has a core diameter of 50 μm, a fiber outer diameter of 125 μm,
It is made of focused multimode optical fiber with a numerical aperture (NA) of 0.2.

伝送路光フアイバ59を伝搬した光は光分岐回
路204へ入力する。光分岐回路204は回折格
子型の分岐回路であつて、その入力側には伝送路
光フアイバ59が接続され、また出力側にはコア
径が100μm、N.A.が0.25のステツプ型マルチモ
ード光フアイバである第9〜第14の光フアイバ6
1〜66が接続されていて、伝送路光フアイバ5
9の出力のλ〜λの波長の光を分岐して第1
〜第6の光受信機101〜106にそれぞれ導い
ている。
The light propagated through the transmission line optical fiber 59 is input to the optical branch circuit 204 . The optical branch circuit 204 is a diffraction grating type branch circuit, and a transmission line optical fiber 59 is connected to its input side, and a step type multimode optical fiber with a core diameter of 100 μm and an NA of 0.25 is connected to its output side. Certain 9th to 14th optical fibers 6
1 to 66 are connected, and the transmission line optical fiber 5
9 output light with wavelengths λ 1 to λ 6 is split into the first
~6th optical receivers 101 to 106, respectively.

第1〜第6の光受信機101〜106において
は、第9〜第14の光フアイバ61〜66の出力光
を第7〜第12の結合回路71〜76で第1〜第6
の光検出器81〜86にそれぞれ入力させ、ここ
で電気信号に変換したのち、第1〜第6の受信回
路91〜96で増幅等を行ない、第1〜第6の電
気信号出力端子111〜116に送出している。
第1〜第6の光検出器81〜86には受光径が
300μmφのSi−アバランシエフオトダイオード
が用いられている。
In the first to sixth optical receivers 101 to 106, the output lights from the ninth to fourteenth optical fibers 61 to 66 are connected to the first to sixth optical fibers by the seventh to twelfth coupling circuits 71 to 76.
are input to the photodetectors 81 to 86, respectively, where they are converted into electrical signals, and then amplified by the first to sixth receiving circuits 91 to 96, and output to the first to sixth electrical signal output terminals 111 to 111. 116.
The first to sixth photodetectors 81 to 86 each have a receiving diameter.
A Si avalanche photodiode with a diameter of 300 μm is used.

以上の説明から分るように、この波長多重光フ
アイバ伝送システムにおける光合波回路を要約し
て説明すると、波長依存性のある光多重回路と、
波長依存性のない光多重回路の組み合せで構成さ
れており、この場合第1の光多重回路では1つお
きの波長の光を波長多重し、第2の光多重回路で
は残りの波長の光を波長多重したのち、これら第
1、第2の光多重回路の出力光を波長依存性のな
い光多重回路で多重するようになつている。従つ
て伝送される光の波長間隔は第1、第2の光多重
回路各々で波長多重される光の波長間隔の1/2に
出来るから、第1、第2の光多重回路各々の使用
波長範囲とほぼ同等の使用波長範囲で第1、第2
の光多重回路各々が多重可能なチヤンネル数の2
倍のチヤンネル数を多重伝送することが出来る。
一方これを別の言い方をすると、伝送するチヤン
ネル数を一定とすれば、使用波長範囲は約1/2に
低減出来るから、伝送路光フアイバの損失の小さ
い波長範囲を使うことが出来るので、伝送路距離
が長く出来る。
As can be seen from the above explanation, the optical multiplexing circuit in this wavelength division multiplexing optical fiber transmission system can be summarized as: a wavelength-dependent optical multiplexing circuit;
It consists of a combination of optical multiplexing circuits with no wavelength dependence. In this case, the first optical multiplexing circuit wavelength-multiplexes the light of every other wavelength, and the second optical multiplexing circuit wavelength-multiplexes the light of the remaining wavelengths. After wavelength multiplexing, the output lights of the first and second optical multiplexing circuits are multiplexed by an optical multiplexing circuit that is not wavelength dependent. Therefore, since the wavelength interval of the transmitted light can be made 1/2 of the wavelength interval of the light wavelength multiplexed by each of the first and second optical multiplexing circuits, the wavelength used by each of the first and second optical multiplexing circuits is The first and second wavelength ranges are approximately the same as the range.
The number of channels that can be multiplexed by each optical multiplexing circuit is 2.
It is possible to multiplex transmit twice the number of channels.
On the other hand, to put this in another way, if the number of transmission channels is constant, the wavelength range used can be reduced to about 1/2, so it is possible to use a wavelength range with less loss in the optical fiber for transmission. The road distance can be increased.

次にシステムの性能を具体的に説明すると第1
の光多重回路201、第2の光多重回路202、
および第3の光多重回路203の挿入損失は各々
約1dB、光分波回路204の挿入損失は約1.5dB
であつたので、光合波分波回路系の挿入損失は合
計で約3.5dBであつた。また、第1、第2の光多
重回路201,202各々に必要とされる波長範
囲は、これら光多重回路各々で多重されるチヤン
ネルの波長間隔が20nmなので、40nm(20nm×
2)に20nmの余裕を考えて合計では各々60nm
になる。なお、伝送路光フアイバ59が使用され
る波長範囲は、伝送される各チヤンネルの波長間
隔が10nmなので、50nm(10nm×5)に10nm
の余裕を考えて60nmになる。伝送路光フアイバ
59の損失は波長がλ=840nmのチヤンネル
に対して最も大きく、約2.8dB/Kmであつた。
Next, I will explain the performance of the system in detail.
an optical multiplex circuit 201, a second optical multiplex circuit 202,
The insertion loss of the third optical multiplexing circuit 203 is approximately 1 dB, and the insertion loss of the optical demultiplexing circuit 204 is approximately 1.5 dB.
Therefore, the total insertion loss of the optical multiplexing/demultiplexing circuit system was about 3.5 dB. Furthermore, the wavelength range required for each of the first and second optical multiplexing circuits 201 and 202 is 40nm (20nm×
Considering the margin of 20nm in 2), the total is 60nm for each.
become. Note that the wavelength range in which the transmission line optical fiber 59 is used is 10 nm in 50 nm (10 nm x 5) because the wavelength interval of each channel to be transmitted is 10 nm.
Considering the margin, it will be 60nm. The loss of the transmission line optical fiber 59 was greatest for a channel having a wavelength of λ 1 =840 nm, which was approximately 2.8 dB/Km.

一方、第1〜第3の光多重回路からなる光合波
回路系を従来の技術の干渉膜型光多重回路だけで
構成するとすれば、この干渉膜型光多重回路で多
重されるチヤンネルの波長間隔は20nmなので、
この干渉膜型光多重回路に必要とされる波長範囲
は120nmになる。また、伝送路光フアイバ59
が使用される波範囲も干渉膜型光多重回路に必要
な波長範囲に等しい120nmになる。
On the other hand, if the optical multiplexing circuit system consisting of the first to third optical multiplexing circuits is constructed only from conventional interference film type optical multiplexing circuits, then the wavelength interval of the channels multiplexed by the interference film type optical multiplexing circuits is 20nm, so
The wavelength range required for this interference film type optical multiplex circuit is 120 nm. In addition, the transmission path optical fiber 59
The wavelength range used is also 120 nm, which is the same wavelength range required for interference film type optical multiplex circuits.

一般に広い波長範囲で干渉膜の損失を小さくす
ることはリツプル等の影響で難かしいために、干
渉膜型光多重回路に必要な波長範囲が広いと挿入
損失が大きくなる。例えばチヤンネル数が6、波
長間隔が20nm、波長範囲が120nmの場合の800n
m帯干渉膜型光多重回路の挿入損失は約4dBの値
になる。また、伝送路光フアイバ59が使用され
る波長範囲が広いとその損失の大きい波長領域も
使わなければならなくなり、或るチヤンネルに対
しては伝送路光フアイバ59の損失が大きくな
る。例えば、第1〜第6の半導体レーザの出力光
の波長λ,λ,………λを790nm、810n
m、830nm、850nm、870nm、890nmにそれぞ
れ設定すると、伝送路光フアイバの損失はλ
790nmのチヤンネルに対して最も大きくて約
3.5dB/Kmになる。
Generally, it is difficult to reduce the loss of an interference film over a wide wavelength range due to the effects of ripples, etc. Therefore, if the wavelength range required for an interference film type optical multiplex circuit is wide, the insertion loss increases. For example, 800n when the number of channels is 6, the wavelength interval is 20nm, and the wavelength range is 120nm.
The insertion loss of an m-band interference film type optical multiplex circuit is approximately 4 dB. Furthermore, if the wavelength range in which the transmission line optical fiber 59 is used is wide, a wavelength range with a large loss must also be used, and the loss of the transmission line optical fiber 59 becomes large for a certain channel. For example, the wavelengths λ 1 , λ 2 , ...... λ 6 of the output lights of the first to sixth semiconductor lasers are set to 790 nm, 810 nm, etc.
m, 830nm, 850nm, 870nm, and 890nm, respectively, the loss of the transmission line optical fiber is λ 1 =
The largest for the 790nm channel is approximately
It becomes 3.5dB/Km.

以上述べたように、本実施例の波長多重光フア
イバ伝送システムでは、光合波分波回路系の挿入
損失が従来よりも約2dB小さく出来た。また、伝
送路光フアイバが使用される波長領域が50nm狭
くなつたので、伝送路光フアイバの損失が最も大
きいチヤンネルでは、伝送路光フアイバの損失が
約3.5dB/Kmから約2.8dB/Kmに低下した。これ
らのために、例えばビツトレイトが100Mb/sの
場合には、伝送路距離は従来約10Kmであつたの
が、本実施例の構成をとることにより約13Kmと約
3Km長くすることが出来た。
As described above, in the wavelength division multiplexing optical fiber transmission system of this embodiment, the insertion loss of the optical multiplexing/demultiplexing circuit system can be reduced by about 2 dB compared to the conventional one. In addition, the wavelength range in which transmission line optical fibers are used has been narrowed by 50 nm, so in channels where transmission line optical fibers have the highest loss, the transmission line optical fiber loss has decreased from approximately 3.5 dB/Km to approximately 2.8 dB/Km. decreased. For these reasons, when the bit rate is 100 Mb/s, for example, the transmission line distance, which was conventionally about 10 km, can be lengthened by about 3 km to about 13 km by adopting the configuration of this embodiment.

なお、以上の実施例では伝送路光フアイバ59
にコア径が50μm、N.A.が0.2の集束型マルチモ
ード光フアイバを使用したが、コア径が約10μm
の単一モード光フアイバ等他のパラメータの光フ
アイバでもよい。また、第3の光多重回路203
として偏波面光多重回路を使用したが、波長依存
性のないものなら何でもよい。例えば昭和53年3
月5日発行の昭和53年度電子通信学会総合全国大
会講演論文集分冊4の第4−112頁、第855番に鹿
田他により提案された複レンズ型光多重回路のよ
うなものであつてもよい。そして、このように第
3の光多重回路203が偏波面光多重回路でない
場合には、第1〜第8の光フアイバ51〜58に
は偏波面保存光フアイバを特に使用しなくてもよ
い。
In addition, in the above embodiment, the transmission path optical fiber 59
We used a focused multimode optical fiber with a core diameter of 50 μm and an NA of 0.2, but the core diameter was approximately 10 μm.
Optical fibers of other parameters may also be used, such as single mode optical fibers. Further, the third optical multiplexing circuit 203
Although a polarization plane optical multiplexing circuit was used as the method, any circuit without wavelength dependence may be used. For example, March 1973
Even if it is something like the double lens type optical multiplex circuit proposed by Shikada et al. in Volume 4 of the Proceedings of the National Conference of the Institute of Electronics and Communication Engineers published on May 5th, 1978, page 4-112, number 855. good. If the third optical multiplexing circuit 203 is not a polarization optical multiplexing circuit as described above, it is not necessary to use polarization maintaining optical fibers for the first to eighth optical fibers 51 to 58.

また、第1〜第6の半導体レーザ31〜36は
800nm帯の光を出力するAlGaAs半導体レーザで
あるとしたが、半導体レーザの材料はInGaAsP
のような他の材料であつてもよいし、また波長帯
も1μm帯のような他の波長帯であつてもよい。
Moreover, the first to sixth semiconductor lasers 31 to 36 are
Although it is an AlGaAs semiconductor laser that outputs light in the 800 nm band, the material of the semiconductor laser is InGaAsP.
It may be made of other materials such as, and the wavelength band may be another wavelength band such as the 1 μm band.

更に伝送チヤンネル数は6チヤンネルとした
が、特に6チヤンネルに限定されるものではな
く、3チヤンネル以上であれば何チヤンネルであ
つてもよい。これと関連して第1〜第6の半導体
レーザ31〜36の出力光の波長の波長間隔は
10nmであるとしたが、この波長間隔はチヤンネ
ル数や使用温度範囲での半導体レーザの波長変化
範囲等を考慮して適当に定められてよく、特に上
記の値に限定されるものではない。
Furthermore, although the number of transmission channels is six, it is not particularly limited to six, and may be any number of channels as long as it is three or more. In connection with this, the wavelength interval of the wavelengths of the output lights of the first to sixth semiconductor lasers 31 to 36 is
Although it is assumed that the wavelength interval is 10 nm, this wavelength interval may be appropriately determined in consideration of the number of channels, the wavelength change range of the semiconductor laser in the operating temperature range, etc., and is not particularly limited to the above value.

更にまた、光合波回路は、波長依存性のある2
個の第1、第2の光多重回路201,202と波
長依存性のない第3の光多重回路203の組み合
せで構成されるとしたが、波長依存性のある光多
重回路と波長依存性のない光多重回路との組み合
せはその他にも種々可能である。例えば、チヤン
ネル数が3の場合には、波長がλのチヤンネル
1の光と波長がλのチヤンネル3の光とを波長
依存性のある干渉膜型の光多重回路で波長多重し
たのち、この波長多重された光と波長がλ(但
し、λ<λ<λ)のチヤンネル2の光とを
波長依存性のない光多重回路である偏波面光多重
回路で多重してもよい。
Furthermore, the optical multiplexing circuit has wavelength-dependent
It is assumed that the configuration is composed of a combination of first and second optical multiplexing circuits 201 and 202 and a third optical multiplexing circuit 203 that has no wavelength dependence. Various other combinations with optical multiplex circuits are also possible. For example, when the number of channels is 3, after wavelength-multiplexing the light of channel 1 with a wavelength of λ 1 and the light of channel 3 with a wavelength of λ 3 using a wavelength-dependent interference film type optical multiplexing circuit, Even if this wavelength-multiplexed light and the light of channel 2 whose wavelength is λ 2 (however, λ 1 < λ 2 < λ 3 ) are multiplexed by a polarization plane optical multiplexing circuit, which is an optical multiplexing circuit without wavelength dependence, good.

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

第1図はこの発明による波長多重光フアイバ伝
送システムの最も好ましい実施例の構成を示すブ
ロツク図である。 記号の説明:1〜6は光送信機、11〜16は
電気信号入力端子、21〜26は送信回路、31
〜36は半導体レーザ、41〜46は結合回路、
51〜58は光フアイバ、59は伝送路光フアイ
バ、61〜66は光フアイバ、71〜76は結合
回路、81〜86は光検出器、91〜96は受信
回路、101〜106は光受信機、111〜11
6は電気信号出力端子、201〜203は光多重
回路、204は光分波回路をそれぞれあらわして
いる。
FIG. 1 is a block diagram showing the configuration of the most preferred embodiment of the wavelength division multiplexing optical fiber transmission system according to the present invention. Explanation of symbols: 1 to 6 are optical transmitters, 11 to 16 are electrical signal input terminals, 21 to 26 are transmission circuits, 31
~36 is a semiconductor laser, 41~46 is a coupling circuit,
51 to 58 are optical fibers, 59 are transmission line optical fibers, 61 to 66 are optical fibers, 71 to 76 are coupling circuits, 81 to 86 are photodetectors, 91 to 96 are receiving circuits, and 101 to 106 are optical receivers. , 111-11
Reference numeral 6 represents an electrical signal output terminal, 201 to 203 represent an optical multiplexing circuit, and 204 represents an optical demultiplexing circuit.

Claims (1)

【特許請求の範囲】[Claims] 1 互いに発振波長の異なる少なくとも3個の半
導体レーザ、これら半導体レーザの出力光の波長
多重を行う光合波手段、波長多重された光を伝搬
する伝送路光フアイバ、伝播された光を波長毎に
分波する分波回路、および分波した各波長の光を
検出する光検出器を含む光フアイバ伝送システム
において、前記光合波手段が、前記半導体レーザ
の出力光を入力とし、少くとも1つの波長依存性
のある光多重回路を含む光多重手段と、前記少く
とも1つの波長依存性のある光多重回路の出力及
び他の波長依存性のある光多重回路の出力又は前
記入力した半導体レーザの出力光を合成して前記
波長多重された光を出力する波長依存性のない光
多重回路とから成り、而して前記光多重手段の波
長依存性のある光多重回路に割当てられる少なく
とも2つのレーザ光の波長が、その大きさの順に
少なくとも1つはなれていることを特徴とする波
長多重光フアイバ伝送システム。
1 At least three semiconductor lasers with different oscillation wavelengths, an optical multiplexing means for wavelength-multiplexing the output lights of these semiconductor lasers, a transmission line optical fiber for propagating the wavelength-multiplexed light, and a means for separating the propagated light into wavelengths. In an optical fiber transmission system including a demultiplexing circuit that generates a wave, and a photodetector that detects the demultiplexed light of each wavelength, the optical multiplexing means inputs the output light of the semiconductor laser and transmits at least one wavelength-dependent light. an optical multiplexing means including a wavelength-dependent optical multiplex circuit, and an output of the at least one wavelength-dependent optical multiplex circuit and an output of another wavelength-dependent optical multiplex circuit or output light of the input semiconductor laser; and a wavelength-independent optical multiplexing circuit that synthesizes the wavelength-multiplexed light and outputs the wavelength-multiplexed light. A wavelength multiplexing optical fiber transmission system characterized in that the wavelengths are separated by at least one wavelength in order of size.
JP56168545A 1981-10-23 1981-10-23 Wavelength multiplex optical fiber transmission system Granted JPS5870652A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56168545A JPS5870652A (en) 1981-10-23 1981-10-23 Wavelength multiplex optical fiber transmission system

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56168545A JPS5870652A (en) 1981-10-23 1981-10-23 Wavelength multiplex optical fiber transmission system

Publications (2)

Publication Number Publication Date
JPS5870652A JPS5870652A (en) 1983-04-27
JPS6235084B2 true JPS6235084B2 (en) 1987-07-30

Family

ID=15869997

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56168545A Granted JPS5870652A (en) 1981-10-23 1981-10-23 Wavelength multiplex optical fiber transmission system

Country Status (1)

Country Link
JP (1) JPS5870652A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2598574B1 (en) * 1986-05-06 1992-02-28 Matra OPTICAL FREQUENCY MULTIPLEXED DATA TRANSMISSION METHOD AND DEVICE
JP2001333015A (en) 2000-05-22 2001-11-30 Fujitsu Ltd Optical multiplexing device and optical multiplexing method

Also Published As

Publication number Publication date
JPS5870652A (en) 1983-04-27

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