JPS628761B2 - - Google Patents

Info

Publication number
JPS628761B2
JPS628761B2 JP56133818A JP13381881A JPS628761B2 JP S628761 B2 JPS628761 B2 JP S628761B2 JP 56133818 A JP56133818 A JP 56133818A JP 13381881 A JP13381881 A JP 13381881A JP S628761 B2 JPS628761 B2 JP S628761B2
Authority
JP
Japan
Prior art keywords
stimulated
light
optical fiber
optical
transmission line
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
JP56133818A
Other languages
Japanese (ja)
Other versions
JPS5834407A (en
Inventor
Kunihiko Washio
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 JP56133818A priority Critical patent/JPS5834407A/en
Publication of JPS5834407A publication Critical patent/JPS5834407A/en
Publication of JPS628761B2 publication Critical patent/JPS628761B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04BTRANSMISSION
    • H04B10/00Transmission systems employing electromagnetic waves other than radio-waves, e.g. infrared, visible or ultraviolet light, or employing corpuscular radiation, e.g. quantum communication
    • H04B10/25Arrangements specific to fibre transmission
    • H04B10/2507Arrangements specific to fibre transmission for the reduction or elimination of distortion or dispersion
    • H04B10/2537Arrangements specific to fibre transmission for the reduction or elimination of distortion or dispersion due to scattering processes, e.g. Raman or Brillouin scattering

Landscapes

  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Engineering & Computer Science (AREA)
  • Computer Networks & Wireless Communication (AREA)
  • Signal Processing (AREA)
  • Optical Couplings Of Light Guides (AREA)
  • Optical Communication System (AREA)
  • Light Guides In General And Applications Therefor (AREA)

Description

【発明の詳細な説明】 本発明は光伝送路に係り、特に超高速・大容量
の情報を長距離伝送させるのに適した高出力光伝
送路に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an optical transmission line, and particularly to a high-power optical transmission line suitable for transmitting ultra-high-speed, large-capacity information over long distances.

近年、単一モード光フアイバの低損失化の進展
に伴ない、その低分散な波長域で動作する超高
速・大容量の情報伝送システムの需要が強くな
り、このため伝送路の中継間隔をできるだけ長く
する必要性がしだいに強まつてきた。
In recent years, with the progress in reducing the loss of single-mode optical fibers, there has been a strong demand for ultra-high-speed, large-capacity information transmission systems that operate in the low-dispersion wavelength range. The need to lengthen it gradually became stronger.

ところで、用いる光フアイバの損失の低減には
限度があるので、長距離の光情報伝送には、でき
るだけ高感度な光検出器を用いるとともに、送信
用の光源として高出力なレーザを用いる必要があ
る。
By the way, there is a limit to the reduction of loss in the optical fiber used, so for long-distance optical information transmission, it is necessary to use a photodetector with as high sensitivity as possible and a high-power laser as the light source for transmission. .

しかしながら、光フアイバ中に高出力レーザ光
を伝送させると、誘導ラマン散乱や誘導4光子混
合などの誘導光散乱が生じ易く、ひいては誘導散
乱光が強くなると、信号光の品質を劣化させてし
まうという問題が生じる。従来の光伝送路におい
ては、誘導散乱光の成長を阻止する効果的な方策
が構じられなかつたために、高出力レーザを光源
として用いることができず、これがため中継間隔
の長い光伝送路を敷設することが困難であるとい
う欠点があつた。
However, when high-power laser light is transmitted through an optical fiber, stimulated light scattering such as stimulated Raman scattering and stimulated four-photon mixing tends to occur, and as the stimulated scattered light becomes stronger, the quality of the signal light deteriorates. A problem arises. In conventional optical transmission lines, high-power lasers cannot be used as light sources because no effective measures have been taken to prevent the growth of stimulated scattered light, and this has made it difficult to use optical transmission lines with long relay intervals. The disadvantage was that it was difficult to install.

本発明の目的は、この従来の光伝送路のもつ欠
点を除去し、超高速・大容量の情報を長距離伝送
することができる光伝送路を提供することにあ
る。
SUMMARY OF THE INVENTION An object of the present invention is to provide an optical transmission line that eliminates the drawbacks of the conventional optical transmission line and is capable of transmitting ultra-high-speed, large-capacity information over long distances.

本発明は、複数の光フアイバを直列に接続した
接続個所のうち少なくとも一個所に、誘導散乱光
を大きく成長させないようにするための帯域フイ
ルタを設けたことを特徴とする光伝送路である。
The present invention is an optical transmission line characterized in that a bandpass filter is provided at at least one of the connection points where a plurality of optical fibers are connected in series to prevent stimulated scattered light from growing to a large extent.

本発明によれば、一つの伝送路にて高出力信号
光を遠地点にまで伝送することができるので、そ
の遠端にて信号光を複数の光フアイバに容易に分
岐できることである。従来は、送信端にて信号光
を複数の光フアイバに分岐させ、光フアイバを束
ねて遠端にまで敷設していたが、これに比べる
と、本発明によれば、光フアイバの所要量を大幅
に節減できるので、経済的な光伝送システムが実
現できる。
According to the present invention, high-power signal light can be transmitted to an apogee through one transmission line, so that the signal light can be easily branched into a plurality of optical fibers at the far end. Conventionally, the signal light was branched into multiple optical fibers at the transmitting end, and the optical fibers were bundled and laid down to the far end, but compared to this, the present invention reduces the amount of optical fiber required. Since the cost can be significantly reduced, an economical optical transmission system can be realized.

光フアイバ中に高出力レーザ光を伝送させたと
きに生じる誘導光散乱には誘導ラマン散乱、誘導
ブリユアン散乱、誘導4光子混合などがある。
Stimulated light scattering that occurs when high-power laser light is transmitted through an optical fiber includes stimulated Raman scattering, stimulated Brillouin scattering, stimulated four-photon mixing, and the like.

これらの誘導光散乱は、超高速・大容量の情報
伝送が可能な、コア径が細い単一モード光フアイ
バにおいてとくに生じやすい。
These stimulated light scatterings are particularly likely to occur in single-mode optical fibers with small core diameters, which are capable of ultra-high-speed, large-capacity information transmission.

また、長距離伝送に適した波長1.3〜1.5μm帯
では、1W以下の、それほど強くないレーザ光を
用いても、長尺の光フアイバを伝送させることに
より誘導散乱光が強く発生しやすくなる。
Furthermore, in the wavelength band of 1.3 to 1.5 μm, which is suitable for long-distance transmission, even if a less intense laser beam of 1 W or less is used, the stimulated scattered light is likely to be generated strongly by transmitting through a long optical fiber.

従つて、超高速・大容量の情報を長距離にわた
つて伝送するには、誘導散乱光が強くならないよ
うに何らかの対策を構ずる必要があることがわか
る。
Therefore, it is clear that in order to transmit ultra-high-speed, large-capacity information over long distances, it is necessary to take some measures to prevent stimulated scattered light from becoming strong.

〔単色のレーザ光源を用い、単一の光フアイバ
にレーザ光を伝送させた場合における、誘導光散
乱の発生による信号劣化が避けられる光フアイバ
入力の限界については、アプライド・オプテイク
ス(Applied Optics)、1972年11月号発行の第11
巻第2489頁乃至2494頁、アール・ジー・スミス
(R.G.Smith)氏の論文に記載されている。〕 さて、誘導光散乱のうちで誘導ブリユアン散乱
は、単色なレーザ光源を用いた場合には信号光の
損失の原因ともなりうるが、ブリユアン散乱の利
得帯域幅は100MHz程度と狭いので、マルチ軸モ
ードのレーザ光を用いるなどして信号光のスペク
トル帯域を広帯域化すれば、誘導ブリユアン散乱
の発生のしきい値を高くすることができ、誘導ラ
マン散乱に比べて誘導ブリユアン散乱の寄与は無
視しうるようにできる。また、誘導4光子混合な
るものは、信号光のほかに他波長の光が存在する
ときに、新たにアンチストークス光を発生するな
どによつて、信号光の損失あるいは異なる波長の
信号間のクロストークなどの発生の原因となりう
るが、この誘導4光子混合の成長は、誘導ラマン
散乱の成長を阻止することによつてほぼ十分に抑
止できる。
[For the limits of optical fiber input to avoid signal degradation due to stimulated light scattering when a monochromatic laser light source is used and laser light is transmitted through a single optical fiber, see Applied Optics, No. 11, November 1972 issue
Vol. 2489-2494, in an article by RG Smith. ] Now, among stimulated light scattering, stimulated Brillouin scattering can cause loss of signal light when a monochromatic laser light source is used, but since the gain bandwidth of Brillouin scattering is narrow at about 100 MHz, multi-axis scattering If the spectral band of the signal light is broadened by using a laser beam with different modes, the threshold for the occurrence of stimulated Brillouin scattering can be raised, and the contribution of stimulated Brillouin scattering can be ignored compared to stimulated Raman scattering. I can do it as if it were wet. In addition, stimulated four-photon mixing is caused by the loss of signal light or the crosstalk between signals of different wavelengths due to the generation of new anti-Stokes light when light of other wavelengths is present in addition to signal light. Although the growth of stimulated four-photon mixing can be a cause of talk and the like, the growth of stimulated four-photon mixing can be almost completely suppressed by inhibiting the growth of stimulated Raman scattering.

従つて、本発明の原理的構成は、光フアイバを
複数の区間に分割し、そのうちの一つ以上の接続
個所に帯域フイルタを設けた点にあり、もつて誘
導ラマン散乱を中心とした誘導散乱光を減衰ない
しは光伝送路から取り除くようにし、誘導散乱光
が大きく成長することを阻止するようにしたこと
に特徴がある。
Therefore, the basic structure of the present invention is that an optical fiber is divided into a plurality of sections, and a bandpass filter is provided at one or more connection points of the sections, and stimulated scattering centered on stimulated Raman scattering is achieved. The feature is that the light is attenuated or removed from the optical transmission path to prevent stimulated scattered light from growing significantly.

次に、本発明による高出力光伝送路について、
図面を参照して詳細に説明する。
Next, regarding the high-power optical transmission line according to the present invention,
This will be explained in detail with reference to the drawings.

第1図は、本発明による一実施例の構成を示し
た模式図である。この図において、1は入射光、
2a,2b,2cは光フアイバ、3a,3bは光
フアイバ接続素子、4a,4bは帯域フイルタ、
5a,5bは光フアイバ伝送路から取り出された
誘導散乱光、6は光伝送路出射光である。
FIG. 1 is a schematic diagram showing the configuration of an embodiment according to the present invention. In this figure, 1 is the incident light,
2a, 2b, 2c are optical fibers, 3a, 3b are optical fiber connection elements, 4a, 4b are band filters,
5a and 5b are stimulated scattered lights taken out from the optical fiber transmission line, and 6 is light emitted from the optical transmission line.

この実施例においては、光フアイバ接続素子3
a,3bには特にセルフオツクレンズを用い、ま
た特に多層膜干渉フイルタからなる帯域フイルタ
4a,4bの反射特性を利用して信号光を反射さ
せ、例えば前段の光フアイバ2aから出射する信
号光を後段の光フアイバ2bに効率よく結合する
ようにしている。
In this embodiment, the optical fiber connecting element 3
In particular, self-occurring lenses are used for a and 3b, and the signal light is reflected by using the reflection characteristics of bandpass filters 4a and 4b, which are made of multilayer interference filters. The optical fiber 2b is efficiently coupled to the subsequent optical fiber 2b.

帯域フイルタ4a,4bの特性は、信号光より
も低周波側に高い透過率をもたせ、信号光よりも
100〜1000cm-1程度低周波側に発生する誘導ラマ
ン散乱光を、それが大きく成長しないうちに光伝
送路から効率よく外部に取り除くようにしてい
る。
The characteristics of the bandpass filters 4a and 4b are that they have higher transmittance on the lower frequency side than the signal light, and have higher transmittance than the signal light.
Stimulated Raman scattered light generated on the low frequency side of about 100 to 1000 cm -1 is efficiently removed from the optical transmission path before it grows large.

第2図は、伝送距離と光フアイバ内の光強度と
の関係を示す模式図である。図において、長さ
la,lb,lcは上述した一実施例における光フアイ
バ2a,2b,2cのフアイバ長にそれぞれ対応
する。実線は帯域フイルタを用いた場合における
光強度を示し、21は信号光強度、22は誘導散
乱光強度である。
FIG. 2 is a schematic diagram showing the relationship between transmission distance and light intensity within an optical fiber. In the figure, the length
la, lb, and lc correspond to the fiber lengths of the optical fibers 2a, 2b, and 2c in the above-described embodiment, respectively. The solid line indicates the light intensity when a bandpass filter is used, 21 is the signal light intensity, and 22 is the stimulated scattered light intensity.

また、一点鎖線は、帯域フイルタを用いないで
ストレートに光フアイバ2a,2b………が融着
接続されている場合における光強度を示し、31
は信号光強度、32は誘導散乱光強度である。
In addition, the dashed-dotted line indicates the light intensity when the optical fibers 2a, 2b, etc. are fusion-spliced straight without using a bandpass filter,
is the signal light intensity, and 32 is the stimulated scattered light intensity.

誘導散乱光は指数函数的に急激に成長するの
で、あるしきい値を越えると、信号光の減衰は非
常に顕著に生じる。従つて長距離の信号伝送は、
この場合(従来の場合)、困難である。〔光フアイ
バ中における誘導散乱光の成長過程のうち、とく
に誘導ラマン散乱光の成長過程に関しては、ア
イ・イー・イー・イー・ジヤーナル・オブ・クオ
ンタム・エレクトロニクス(IEEE、Journal of
Quantum Electronics)、1978年5月号発行の、
第14巻、第347頁乃至352頁、ジエイ・オウヤン
(J.Auyeung)氏らの論文に記載されている。〕 第2図から明らかな如く、本発明によれば、誘
導散乱光の急激な成長が効果的に阻止できるの
で、従来よりもはるかに遠距離にまで高出力な信
号光を伝送することができる。
Since the stimulated scattered light grows rapidly exponentially, when a certain threshold value is exceeded, the signal light is attenuated very significantly. Therefore, long-distance signal transmission is
In this case (conventional case), it is difficult. [The growth process of stimulated scattered light in optical fibers, especially the growth process of stimulated Raman scattered light, is described in the IEEE Journal of Quantum Electronics (IEEE, Journal of Quantum Electronics).
Quantum Electronics), May 1978 issue,
It is described in the paper by J. Auyeung et al., Volume 14, pages 347 to 352. ] As is clear from FIG. 2, according to the present invention, the rapid growth of stimulated scattered light can be effectively prevented, so high-power signal light can be transmitted over a much longer distance than before. .

高出力信号光として、例えば1.3μmYAGレー
ザ光を用い、光フアイバとして低分散・低損失な
単一モード光フアイバを用いても良く、これによ
り超高速・大容量の情報の長距離伝送が可能にな
る。
For example, a 1.3μm YAG laser beam may be used as the high-output signal light, and a low-dispersion, low-loss single-mode optical fiber may be used as the optical fiber, which enables ultra-high-speed, large-capacity, long-distance transmission of information. Become.

光フアイバの接続個所に帯域フイルタを介在さ
せるためには、このための光接続回路による信号
光の減衰はある程度避けられない。しかし、従来
よりもはるかに高出力なレーザ光を伝送できるこ
とによる伝送距離の増大効果による利点ははかり
知れないほど大きい。
In order to interpose a bandpass filter at the connection point of the optical fiber, attenuation of the signal light by the optical connection circuit for this purpose is unavoidable to some extent. However, the advantage of increasing the transmission distance by being able to transmit laser light with much higher output than before is immeasurably large.

光フアイバの伝送損失により信号光強度はしだ
いに減衰するので信号光強度が弱まれば、光フア
イバの単長を長くし、送信端より遠方側では光伝
送路内に介在させる帯域フイルタの単位フアイバ
長あたりの数を減らすことができる。
The signal light intensity gradually attenuates due to the transmission loss of the optical fiber, so if the signal light intensity weakens, the single length of the optical fiber is lengthened, and a unit fiber of a bandpass filter is inserted in the optical transmission line on the side far from the transmitting end. The number per length can be reduced.

以上述べたごとく、本発明によれば、低分散・
低損失な光フアイバに高出力なレーザ光を伝送す
ることができるので、超高速・大容量の情報を長
距離にわたつて伝送することができる高出力光伝
送路が得られる。
As described above, according to the present invention, low dispersion and
Since high-power laser light can be transmitted through a low-loss optical fiber, a high-power optical transmission line that can transmit ultra-high-speed, large-capacity information over long distances can be obtained.

なお、この発明は、上述の実施例に見られる構
成のみに限定されることなく、いくつかの変形が
考えられる。例えば、帯域フイルタとして、多層
膜干渉フイルタの代りに、回折格子形反射鏡を用
いることができる。また、多層膜干渉フイルタを
用いる代りに、波長選択性の吸収体を用いて誘導
散乱光のみを選択的に減衰させるようにしても差
しつかえない。
Note that the present invention is not limited to only the configurations seen in the above-described embodiments, and several modifications are possible. For example, a diffraction grating reflector can be used as the bandpass filter instead of a multilayer interference filter. Furthermore, instead of using a multilayer interference filter, a wavelength-selective absorber may be used to selectively attenuate only the stimulated scattered light.

【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模式
図である。第2図は伝送距離と光フアイバ内の光
強度との関係を示す模式図である。 尚図において、1……入射光、2a,2b,2
c……光フアイバ、3a,3b……光フアイバ接
続素子、4a,4b……帯域フイルタ、5a,5
b……光フアイバ伝送路から取り出された誘導散
乱光、6……光伝送路出射光、la,lb,lc……フ
アイバ長、21,22……帯域フイルタを用いた
ときのそれぞれ信号光強度、誘導散乱光強度、3
1,32……帯域フイルタを用いないときのそれ
ぞれ信号光強度、誘導散乱光強度である。
FIG. 1 is a schematic diagram showing the configuration of an embodiment according to the present invention. FIG. 2 is a schematic diagram showing the relationship between transmission distance and light intensity within an optical fiber. In the figure, 1...incident light, 2a, 2b, 2
c... Optical fiber, 3a, 3b... Optical fiber connection element, 4a, 4b... Bandwidth filter, 5a, 5
b... Stimulated scattered light taken out from the optical fiber transmission line, 6... Light emitted from the optical transmission line, la, lb, lc... Fiber length, 21, 22... Signal light intensity when using band filters, respectively. , stimulated scattered light intensity, 3
1, 32...These are the signal light intensity and stimulated scattered light intensity, respectively, when no bandpass filter is used.

Claims (1)

【特許請求の範囲】[Claims] 1 複数の光フアイバを直列に接続してなる光伝
送路において、前記光フアイバの接続個所のうち
の少なくとも一個所に、誘導散乱光を大きく成長
させないようにするための帯域フイルタを設けた
ことを特徴とする光伝送路。
1. In an optical transmission line formed by connecting a plurality of optical fibers in series, a bandpass filter is provided at at least one of the connection points of the optical fibers to prevent the stimulated scattered light from growing to a large extent. Characteristic optical transmission line.
JP56133818A 1981-08-25 1981-08-25 Light transmission line Granted JPS5834407A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56133818A JPS5834407A (en) 1981-08-25 1981-08-25 Light transmission line

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56133818A JPS5834407A (en) 1981-08-25 1981-08-25 Light transmission line

Publications (2)

Publication Number Publication Date
JPS5834407A JPS5834407A (en) 1983-02-28
JPS628761B2 true JPS628761B2 (en) 1987-02-24

Family

ID=15113754

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56133818A Granted JPS5834407A (en) 1981-08-25 1981-08-25 Light transmission line

Country Status (1)

Country Link
JP (1) JPS5834407A (en)

Families Citing this family (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FI74371C (en) * 1982-06-04 1988-01-11 British Telecomm Optical transmission.
JP2855525B2 (en) * 1987-07-08 1999-02-10 国際電信電話株式会社 Optical fiber communication system
US6388800B1 (en) * 2000-06-30 2002-05-14 Lucent Technologies Inc. Raman amplifier with gain enhancement from optical filtering
US6466712B1 (en) * 2000-08-21 2002-10-15 Lucent Technologies Inc. Optical transmission link incorporating highpass optical filtering
US6898351B2 (en) * 2000-11-07 2005-05-24 Photon-X, Llc Optical fiber transmission systems with suppressed light scattering

Also Published As

Publication number Publication date
JPS5834407A (en) 1983-02-28

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