JPH04322228A - Optical fiber amplifier - Google Patents
Optical fiber amplifierInfo
- Publication number
- JPH04322228A JPH04322228A JP9052491A JP9052491A JPH04322228A JP H04322228 A JPH04322228 A JP H04322228A JP 9052491 A JP9052491 A JP 9052491A JP 9052491 A JP9052491 A JP 9052491A JP H04322228 A JPH04322228 A JP H04322228A
- Authority
- JP
- Japan
- Prior art keywords
- optical fiber
- light
- mode
- light source
- excitation
- 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
Links
- 239000013307 optical fiber Substances 0.000 title claims abstract description 39
- 230000005284 excitation Effects 0.000 claims abstract description 19
- 239000000835 fiber Substances 0.000 claims abstract description 14
- 229910052761 rare earth metal Inorganic materials 0.000 claims abstract description 10
- 230000002194 synthesizing effect Effects 0.000 claims 1
- 230000003287 optical effect Effects 0.000 abstract description 16
- 150000002910 rare earth metals Chemical class 0.000 abstract description 8
- 230000001427 coherent effect Effects 0.000 abstract description 4
- 238000005086 pumping Methods 0.000 description 5
- 230000003321 amplification Effects 0.000 description 3
- 238000003491 array Methods 0.000 description 3
- 238000004891 communication Methods 0.000 description 3
- 238000003199 nucleic acid amplification method Methods 0.000 description 3
- 230000000694 effects Effects 0.000 description 2
- 238000005516 engineering process Methods 0.000 description 2
- 238000004519 manufacturing process Methods 0.000 description 2
- 239000000758 substrate Substances 0.000 description 2
- 229910052691 Erbium Inorganic materials 0.000 description 1
- 230000005540 biological transmission Effects 0.000 description 1
- 238000005253 cladding Methods 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- UYAHIZSMUZPPFV-UHFFFAOYSA-N erbium Chemical compound [Er] UYAHIZSMUZPPFV-UHFFFAOYSA-N 0.000 description 1
- 230000005281 excited state Effects 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- 229920000515 polycarbonate Polymers 0.000 description 1
- 239000004417 polycarbonate Substances 0.000 description 1
- 238000006116 polymerization reaction Methods 0.000 description 1
- 238000012827 research and development Methods 0.000 description 1
- 239000004065 semiconductor Substances 0.000 description 1
Abstract
Description
【0001】0001
【産業上の利用分野】本発明は、コア部に希土類をドー
プした光ファイバを適当な光源によって励起して反転準
位を得、それによって光を増幅する光ファイバ増幅器に
関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an optical fiber amplifier in which an optical fiber whose core is doped with a rare earth element is excited by a suitable light source to obtain an inversion level, thereby amplifying light.
【0002】0002
【従来の技術】近年、希士類特にエルビウム(Er)を
ドープした光ファイバを用いた光増幅器が著しい進歩を
とげている(たとえば、中沢,「Erドープ光ファイバ
ーによる光増幅とその応用」,応用物理,第59巻,第
9号(1990),P1175〜1192、堀口,「光
ファイバ増幅器」,光学,第19巻,第5号(1990
)、P276〜282等参照)。[Background Art] In recent years, optical amplifiers using optical fibers doped with rare elements, especially erbium (Er), have made remarkable progress (for example, Nakazawa, "Optical amplification using Er-doped optical fibers and its applications", Physics, Vol. 59, No. 9 (1990), P1175-1192, Horiguchi, "Optical Fiber Amplifier", Optics, Vol. 19, No. 5 (1990)
), see pages 276-282, etc.).
【0003】これらのErドープファイバ増幅器の研究
開発は、主に長距離の光通信を念頭に置いて行われてい
るので、シングルモードの光ファイバ系の光増幅が中心
課題となっている。Research and development of these Er-doped fiber amplifiers has been carried out mainly with long-distance optical communications in mind, and therefore optical amplification of single-mode optical fiber systems has become a central issue.
【0004】しかし、光増幅は、たとえば、光LAN(
local areanetwork)や光CATV(
community antennatelevisi
on)系に於ける分配損失を補うというような用途にも
有望である。このような近距離の光通信ネットワークに
は、取り扱いの容易なマルチモード光ファイバが適して
いる。However, optical amplification is difficult to achieve, for example, in an optical LAN (
local area network) and optical CATV (
community antennaelevisi
It is also promising for applications such as compensating for distribution losses in on) systems. Multimode optical fibers, which are easy to handle, are suitable for such short-distance optical communication networks.
【0005】[0005]
【発明が解決しようとする課題】光LAN用のマルチモ
ード光ファイバ増幅器の実現を考えると次のような問題
がある。Problems to be Solved by the Invention When considering the realization of a multimode optical fiber amplifier for optical LAN, the following problems arise.
【0006】1)マルチモード光ファイバは、当然なが
ら多数のモードがあり、たとえば、コア径60μm、N
A(開口数)=0.2のグレーデッドインデックス型フ
ァイバでは、立ち得るモード数は500にもなる(たと
えば、野田, 「光ファイバ伝送」, 電子通信学会(
1978), P42参照。)。任意のモードに対して
等しい利得を得るには、コア内部が均一に励起されなけ
ればならない。言い換えれば、励起光を各モード均一に
照射しなければならない。しかしながら、レーザ光はコ
ヒーレンス(可干渉性)を有しているので、励起光源に
レーザ光源を用いた場合、励起光を各モード均一に照射
することは実現困難である。1) Multimode optical fiber naturally has many modes, for example, a core diameter of 60 μm, N
In a graded index fiber with A (numerical aperture) = 0.2, the number of possible modes is as high as 500 (for example, Noda, "Optical fiber transmission", Institute of Electronics and Communication Engineers (IEICE)).
1978), p. 42. ). To obtain equal gain for any mode, the interior of the core must be uniformly excited. In other words, each mode must be uniformly irradiated with excitation light. However, since laser light has coherence, when a laser light source is used as an excitation light source, it is difficult to uniformly irradiate each mode with excitation light.
【0007】2)マルチモードファイバは、コア径が5
0〜60μmと大きく、コア径が10μm程のシングル
モードファイバに比べ、同じ励起密度を得るには数十倍
の励起光を照射する必要がある。2) The multimode fiber has a core diameter of 5
Compared to a single mode fiber, which has a large diameter of 0 to 60 μm and a core diameter of about 10 μm, it is necessary to irradiate several tens of times as much excitation light to obtain the same excitation density.
【0008】本発明は、前記問題点を解決するために案
出されたものであって、マルチモード光ファイバを十分
な励起密度で励起できるようにすることを目的とする。
また、本発明は、コヒーレンントな光源を使用しつつ、
マルチモードファイバのコア部の励起状態を平準化する
ことを目的とする。The present invention was devised to solve the above-mentioned problems, and an object of the present invention is to make it possible to pump a multimode optical fiber with sufficient pumping density. Further, the present invention uses a coherent light source and
The purpose is to equalize the excited state of the core of a multimode fiber.
【0009】[0009]
【課題を解決するための手段】本発明の光ファイバ増幅
器は、コアに希土類をドープしたマルチモード光ファイ
バと、複数の光源からの励起光を合成して前記マルチモ
ード光ファイバに供給して該マルチモード光ファイバを
励起する光合成手段とを有する。[Means for Solving the Problems] The optical fiber amplifier of the present invention combines a multimode optical fiber whose core is doped with rare earth and pumping light from a plurality of light sources and supplies the combined pump light to the multimode optical fiber. and a light combining means for exciting the multimode optical fiber.
【0010】0010
【作用】複数の光源からの励起光が合成されることによ
り、励起密度が上昇しマルチモードファイバが十分励起
される。また、光源としてレーザを使用した場合でも、
複数の光源からの励起光が合成されることにより、各励
起光が有するコヒーレンスが減じられる。これにより、
希土類ドープファイバにおいて励起されるモードの数が
統計的に増し、マルチモード動作が可能となる。[Operation] By combining excitation light from a plurality of light sources, the excitation density increases and the multimode fiber is sufficiently excited. Also, even when using a laser as a light source,
By combining excitation light from a plurality of light sources, the coherence of each excitation light is reduced. This results in
The number of modes excited in the rare earth doped fiber is statistically increased, allowing multimode operation.
【0011】[0011]
【実施例】以下、図面を参照しながら実施例に基づいて
本発明の特徴を具体的に説明する。DESCRIPTION OF THE PREFERRED EMBODIMENTS Hereinafter, features of the present invention will be specifically explained based on embodiments with reference to the drawings.
【0012】本発明の光ファイバ増幅器の実施例の概略
の構成を第1図に示す。複数の独立した光源1a,1b
,1cから各入力光ファイバ2a,2b,2cを介して
供給される励起光と、信号入力端3から入力光ファイバ
4を介して供給される入力信号光を、合波器5によって
合波し、光アイソレータ6を通して希土類ドープファイ
バ7を励起する。前記合波器5は、図2に示すように、
ガラス或いはポリカーボネートの基板5a上にイオン選
択或いは選択重合により光導波路5bを形成することに
より構成されている。FIG. 1 shows a schematic configuration of an embodiment of the optical fiber amplifier of the present invention. Multiple independent light sources 1a, 1b
, 1c via the respective input optical fibers 2a, 2b, 2c, and the input signal light supplied from the signal input end 3 via the input optical fiber 4, are multiplexed by a multiplexer 5. , pumps the rare earth doped fiber 7 through the optical isolator 6. The multiplexer 5, as shown in FIG.
It is constructed by forming an optical waveguide 5b on a glass or polycarbonate substrate 5a by ion selection or selective polymerization.
【0013】希土類ドープファイバ7の励起により増幅
された信号光は、狭帯域フィルタ8を介して出力端9に
至り出力信号光が得られる。The signal light amplified by the excitation of the rare earth doped fiber 7 passes through a narrow band filter 8 and reaches an output end 9, where an output signal light is obtained.
【0014】各光源1a,1b,1cは、同一構成を有
しており、光源1aを例に挙げると、たとえば図3に示
すように、通常の半導体レーザダイオード10からの励
起光11を、レンズ12で収束してマルチモードの入力
光ファイバ2aのコア部13に照射する。なお、14は
入力光ファイバ2aのクラッド部である。Each of the light sources 1a, 1b, and 1c has the same configuration. Taking the light source 1a as an example, as shown in FIG. 3, for example, as shown in FIG. 12 and irradiates the core portion 13 of the multimode input optical fiber 2a. Note that 14 is a cladding portion of the input optical fiber 2a.
【0015】上述のように複数の光源1a,1b,1c
からの光を合成して希土類ドープファイバ7を励起する
ことにより、励起されるモードの数が統計的に増す。す
なわち、複数の光源1a,1b,1cからの各光の位相
が互いに異なってくるので、励起されるモードの数は増
す。また、励起光量も、単独光源の場合に比べ増加する
。すなわち、個々にはコヒーレントな複数個の光源から
の光を合成して励起光源とすることにより、全体のコヒ
ーレンス(可干渉性)を低減し、あわせて光量増加を図
っている。As mentioned above, a plurality of light sources 1a, 1b, 1c
The number of excited modes is statistically increased by combining the light from the light source and exciting the rare earth-doped fiber 7. That is, since the phases of the lights from the plurality of light sources 1a, 1b, and 1c become different from each other, the number of excited modes increases. Furthermore, the amount of excitation light also increases compared to the case of a single light source. That is, by combining light from a plurality of individually coherent light sources to form an excitation light source, the overall coherence is reduced, and at the same time, the amount of light is increased.
【0016】次に、光ファイバ増幅器において使用され
る光源の他の構成例を図4に示す。図4に示す例におい
ては、各光源1a,1b,1cとしてレーザダイオード
アレイ15を使用した点が図3に示す光源と異なってい
る。図4に示すように、3個の独立した、すなわち位相
同期していないレーザダイオード15a,15b,15
cを10μm間隔でひとつのチップ上に形成した発光素
子を光源として用いている。各レーザダイオードを位相
同期させないようにするためには、たとえば、各ダイオ
ードを比較的閉じ込め効果の高い光導波路中に入れてや
ればよい。Next, another configuration example of a light source used in an optical fiber amplifier is shown in FIG. The example shown in FIG. 4 differs from the light source shown in FIG. 3 in that a laser diode array 15 is used as each light source 1a, 1b, 1c. As shown in FIG.
A light emitting element formed on one chip at intervals of 10 μm is used as a light source. In order to prevent the laser diodes from being phase-synchronized, for example, each diode may be placed in an optical waveguide with a relatively high confinement effect.
【0017】これにより、3本の入力光ファイバ2a,
2b,2cのそれぞれに対して3個のレーザ光源が配置
されることになる。したがって、合計9個の互いに独立
したレーザ光源からの光を合成して励起光のコヒーレン
スを一層低下させ、かつ光量を増加させることができる
。[0017] As a result, the three input optical fibers 2a,
Three laser light sources are arranged for each of 2b and 2c. Therefore, by combining the lights from a total of nine independent laser light sources, it is possible to further reduce the coherence of the excitation light and increase the amount of light.
【0018】合波器5における合波数をさらに増やせば
、コヒーレンスをさらに低下させ、かつ、光量を増すこ
とができる。アレイの数を増すことについては、光ファ
イバのコア径が50〜60μmmということによって制
約を受けるので、現在の製造技術ではアレイの数をこれ
以上増すことは難しい。但し、製造技術上が向上して、
レーザダイオード間の間隔を10μmより十分短くする
ことができるようになれば、アレイの数を更に増やすこ
とは可能である。If the number of multiplexed waves in the multiplexer 5 is further increased, the coherence can be further reduced and the amount of light can be increased. Increasing the number of arrays is limited by the fact that the core diameter of the optical fiber is 50 to 60 μmm, so it is difficult to increase the number of arrays any further with current manufacturing technology. However, as manufacturing technology improves,
If the distance between laser diodes can be made sufficiently shorter than 10 μm, it is possible to further increase the number of arrays.
【0019】[0019]
【発明の効果】以上に述べたように、本発明においては
、複数の光源からの光を合成してマルチモード希土類ド
ープファイバを励起しているので、光源単体としてレー
ザ等のコヒーレントな光源を使用した場合でも、光のコ
ヒーレンスが低下された状態で励起される。したがって
、励起されるモードの数が増加し、コア部の励起を平準
化することができる。また、光を合成するので励起光量
が増加し、径大なマルチモード光ファイバを十分な励起
密度で励起することができる。[Effects of the Invention] As described above, in the present invention, since the light from multiple light sources is combined to excite the multimode rare earth doped fiber, a coherent light source such as a laser is used as the single light source. Even in this case, the light is excited with reduced coherence. Therefore, the number of excited modes increases, and the excitation of the core can be leveled. Furthermore, since the light is combined, the amount of pumping light increases, and a large-diameter multimode optical fiber can be pumped with sufficient pumping density.
【図1】 本発明の光ファイバ増幅器の全体構成を示
す光配線図である。FIG. 1 is an optical wiring diagram showing the overall configuration of an optical fiber amplifier of the present invention.
【図2】 図1に示す光ファイバ増幅器において使用
される光合波器の構成例を示す概略平面図である。2 is a schematic plan view showing a configuration example of an optical multiplexer used in the optical fiber amplifier shown in FIG. 1. FIG.
【図3】 図1に示す光ファイバ増幅器において使用
される光源の構成例を示す要部拡大図である。3 is an enlarged view of a main part showing an example of the configuration of a light source used in the optical fiber amplifier shown in FIG. 1. FIG.
【図4】 図1に示す光ファイバ増幅器において使用
される光源の他の構成例を示す要部拡大図である。4 is an enlarged view of main parts showing another example of the configuration of a light source used in the optical fiber amplifier shown in FIG. 1. FIG.
1a,1b,1c 光源、2a,2b,2c 入力
光ファイバ、3 信号入力端、4 入力光ファイバ
、5 合波器、5a 基板、5b 導波路、6
光アイソレイータ、7 希土類ドープファイバ、8
狭帯域フィルタ、9 出力端、10 半導体レ
ーザダイオード、11 励起光、12 レンズ、1
3 コア部、14 クラッド部、15 レーザダ
イオードアレイ、15a,15b,15c レーザダ
イオード1a, 1b, 1c light source, 2a, 2b, 2c input optical fiber, 3 signal input end, 4 input optical fiber, 5 multiplexer, 5a substrate, 5b waveguide, 6
Optical isolator, 7 Rare earth doped fiber, 8
Narrowband filter, 9 Output end, 10 Semiconductor laser diode, 11 Pumping light, 12 Lens, 1
3 core part, 14 clad part, 15 laser diode array, 15a, 15b, 15c laser diode
Claims (1)
ド光ファイバと、複数の光源からの励起光を合成して前
記マルチモード光ファイバに供給して該マルチモード光
ファイバを励起する光合成手段とを有する光ファイバ増
幅器。1. A multimode optical fiber having a core doped with a rare earth element, and a light synthesizing means for combining excitation light from a plurality of light sources and supplying the combined excitation light to the multimode optical fiber to excite the multimode optical fiber. fiber optic amplifier.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP9052491A JPH04322228A (en) | 1991-04-22 | 1991-04-22 | Optical fiber amplifier |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP9052491A JPH04322228A (en) | 1991-04-22 | 1991-04-22 | Optical fiber amplifier |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH04322228A true JPH04322228A (en) | 1992-11-12 |
Family
ID=14000824
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP9052491A Pending JPH04322228A (en) | 1991-04-22 | 1991-04-22 | Optical fiber amplifier |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH04322228A (en) |
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1991
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