JPH02308581A - Light amplification - Google Patents

Light amplification

Info

Publication number
JPH02308581A
JPH02308581A JP1128961A JP12896189A JPH02308581A JP H02308581 A JPH02308581 A JP H02308581A JP 1128961 A JP1128961 A JP 1128961A JP 12896189 A JP12896189 A JP 12896189A JP H02308581 A JPH02308581 A JP H02308581A
Authority
JP
Japan
Prior art keywords
light
input
output
optical
monitor
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
JP1128961A
Other languages
Japanese (ja)
Inventor
Kosaku Ota
太田 功作
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
Original Assignee
Furukawa 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 Furukawa Electric Co Ltd filed Critical Furukawa Electric Co Ltd
Priority to JP1128961A priority Critical patent/JPH02308581A/en
Publication of JPH02308581A publication Critical patent/JPH02308581A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/05Construction or shape of optical resonators; Accommodation of active medium therein; Shape of active medium
    • H01S3/06Construction or shape of active medium
    • H01S3/063Waveguide lasers, i.e. whereby the dimensions of the waveguide are of the order of the light wavelength
    • H01S3/067Fibre lasers
    • H01S3/06754Fibre amplifiers
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/10Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating
    • H01S3/13Stabilisation of laser output parameters, e.g. frequency or amplitude
    • H01S3/1301Stabilisation of laser output parameters, e.g. frequency or amplitude in optical amplifiers
    • H01S3/13013Stabilisation of laser output parameters, e.g. frequency or amplitude in optical amplifiers by controlling the optical pumping

Abstract

PURPOSE:To keep a rate of light amplification factor constant by comparing a level ratio of an input monitor light and output monitor light with a reference value whose light is set in advance and by adjusting an output power of excitation light automatically to make the level ratio show the reference value. CONSTITUTION:An input light (a) and an excitation light (b) from an excitation light source 2 are joined through an optical combination device 3, input to an optical fiber amplifier 1, amplified, and outputs an output light (c). A part of the input light (a) is branched at an optical branching device 5, input to an input-side photo/electrical conversion section 21 of the excitation light source 2, converted into an electrical signal, and input to the next division circuit 23. The output light (c) is branched at an optical branching device 4 and input to an output-side photo/electrical conversion section 22 of the excitation light source 2 as an output monitor light (e) to be converted into an electrical signal, and input to a division circuit 23. A level ratio of obtained monitor lights (d), (e) is input to a comparison circuit 24 and compared with a reference voltage which is set at a reference voltage generating section 25. Comparison results are input to the electricity/light conversion section 25 and power of the excitation light (b) is controlled.

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は、希を類添加光ファイバ等の光ファイバ増幅器
に入力される入力光に励起光を注入して、同入力光を増
幅するようにした光増幅方法に関するものであり、光通
信や光計測等に使用されるものである。
Detailed Description of the Invention (Field of Industrial Application) The present invention is directed to amplifying the input light by injecting pumping light into the input light input to an optical fiber amplifier such as a rare-doped optical fiber. This invention relates to an optical amplification method used in optical communication, optical measurement, etc.

(従来技術) 希七類添加光ファイバ等を光ファイバ増幅器として用い
た光増幅方法の主なものとしては第2図に示すようなも
のがある。第2図の光増幅方法は入力光aと励起光源2
からの励起光すとを光合流器3により混合して光ファイ
バ増幅器lに入力し、同光ファイバ増幅itが励起光す
のエネルギーを吸収し、そのエネルギーにより入力光a
を増幅して出力光Cとするものである。
(Prior Art) The main optical amplification method using a heptad-doped optical fiber or the like as an optical fiber amplifier is shown in FIG. 2. The optical amplification method shown in Figure 2 is based on the input light a and the pumping light source 2.
The pumping light A is mixed by the optical combiner 3 and input to the optical fiber amplifier L, which absorbs the energy of the pumping light A, and uses that energy to transform the input light A.
The output light C is amplified.

この光増幅方法では光ファイバ増幅器lにより増幅され
た光がそのまま出力光Cとして取り出されるため5例え
ば光ファイバ増幅器1や励起光源2等の周囲の温度変化
によって励起光パワーが変化したり、光合流、器3の通
過損失が変化したりして同増幅器lの利得係数が変化す
ると、その変化に応じて、入力光aが一定でも出力光の
レベルが変動し、伝送系として不安定になるという問題
があった。
In this optical amplification method, the light amplified by the optical fiber amplifier 1 is extracted as is as the output light C.5 For example, the pumping light power may change due to changes in the surrounding temperature of the optical fiber amplifier 1, the pumping light source 2, etc. If the gain coefficient of amplifier l changes due to a change in the passage loss of amplifier 3, the level of the output light will vary even if the input light a is constant, and the transmission system will become unstable. There was a problem.

ぞでで本件出願人は先に第3図のような光増幅方法を開
発した。これは入力光aと励起光すとを合成して光ファ
イバ増幅器1に入力し、前記入力光aを同増幅器lによ
り増幅しぞ同増幅器lから出力光Cとして出力し、その
一部を光分岐器4により取り出してモニタkeとし、こ
のモニタ光eを光・電気変換器Itにより電気信号に変
換し、それを電気信号増幅器12で増幅し、この増幅さ
れた信号が定電流源13からの一定電流と差動増幅器1
4において加算し、この加算した定電流に塙づいて光@
調整された励起光すが電気・光変換部(励起光出力部)
15から発生され、この励起光すにより光ファイバ増幅
器lの利得を調整するようにしたものである。
The applicant of the present invention previously developed an optical amplification method as shown in Figure 3. This combines input light a and pumping light S and inputs it into optical fiber amplifier 1, and the input light a is amplified by amplifier l, which outputs it as output light C, and part of it is optically The monitor light e is taken out by a splitter 4 and used as a monitor ke, and this monitor light e is converted into an electrical signal by an optical-to-electrical converter It, which is amplified by an electrical signal amplifier 12, and this amplified signal is output from a constant current source 13. Constant current and differential amplifier 1
4, and the added constant current is followed by light @
Adjusted excitation light Suga electrical/optical conversion section (excitation light output section)
15, and the gain of the optical fiber amplifier l is adjusted by this pumping light.

(発明が解決しようとする課題) しかし、前記光増幅方法では光ファイバ増幅器【の利得
そのものが調整されるため、入力光レベルが変化した場
合でも出力光レベルが一定になる。このため前記光増幅
方法は、入力光レベルの変化に依存せずに常に利得が一
定な光増幅器が要求される測定器分野では使用すること
が出来ないという問題があった。
(Problem to be Solved by the Invention) However, in the optical amplification method, the gain itself of the optical fiber amplifier is adjusted, so even if the input light level changes, the output light level remains constant. For this reason, the optical amplification method described above cannot be used in the field of measuring instruments, which requires an optical amplifier whose gain is always constant regardless of changes in the input light level.

(発明の目的) 本発明の目的は、光ファイバ増幅器や励起光源等の周囲
の温度変化によって、励起光パワーが変化したり、光合
流器の通過損失が変化したりしても、また入力光が変化
しても光ファイバ増幅器の利得が常に一定になるように
した光増幅方法を提供することにある。
(Objective of the Invention) The object of the present invention is to prevent the input light from changing even if the pumping light power changes or the passage loss of the optical combiner changes due to temperature changes around the optical fiber amplifier or pumping light source. An object of the present invention is to provide an optical amplification method in which the gain of an optical fiber amplifier is always constant even when the gain of an optical fiber amplifier changes.

(間開点を解決するための手段) 本発明の光増幅方法は第1図のように、入力光aと励起
光すとを合成して光ファイバ増幅itに入力し、前記入
力光aを同増幅器lにより増幅して出力光〇とするよう
にした光増幅方法において、前記入力光aの一部を取り
出して大力モニタ光dとし、前記出力光Cの一部を取り
出して出力モニタ光eとし、両モニタ光d、eのレベル
比をr−め設定されている基準値と比較して、同レベル
比がJii l (INと一致するように励起光すの出
力パワーを自動調整するようにしたものである。
(Means for solving gap gap) The optical amplification method of the present invention, as shown in FIG. In the optical amplification method, a part of the input light a is taken out as the output light d and a part of the output light C is taken out as the output monitor light e. Then, the level ratio of both monitor lights d and e is compared with the reference value set r-me, and the output power of the pump light is automatically adjusted so that the same level ratio matches Jii l (IN). This is what I did.

(作用) 本発明の光増幅方法は、入力光aの一部を入力モニタ光
dとし、出力光Cの一部を出力モニタ光eとし1両モニ
タ光d、eのレベル比が予め設定されている基準値と一
致するように、励起光すの出力パワーを自動調整される
ため、先ファイバ増幅klや励起光源2等の周囲温度の
変化により励起光パワーが変化したり、光合流器3の通
過損失が変化したりしても、また、入力光が変化しても
先ファイバ増幅器lの利得は常に一定となる。
(Function) In the optical amplification method of the present invention, a part of the input light a is used as the input monitor light d, a part of the output light C is used as the output monitor light e, and the level ratio of the two monitor lights d and e is set in advance. Since the output power of the pumping light is automatically adjusted to match the reference value set by Even if the transmission loss of the fiber amplifier l changes, or even if the input light changes, the gain of the fiber amplifier l remains constant.

ちなみに、入力モニタ光dと出力モニタ光eの比をDと
し、予め設定された値をAとすると、D<Aのときは励
起光を増やす。
Incidentally, if the ratio of the input monitor light d and the output monitor light e is D and the preset value is A, the pumping light is increased when D<A.

D>Aのときは励起光を減らす。When D>A, reduce the excitation light.

D=Aのときは励起光をそのまま維持する。When D=A, the excitation light is maintained as it is.

ことにより、D=Aを保つ。By doing so, D=A is maintained.

(実施例) 第1図は本発明の光増幅方法の一例であり、同図では入
力光aと励起光源2からの励起光すとが光合流器3また
は光合波器により合流されて、希土類元素添加光ファイ
バを用いた光ファイバ増幅2”51に人力される。この
光ファイバ増幅器lはエルビウムを添加した光ファイバ
でも半導体レーザを用いた進行波型光増幅器でも良い。
(Example) FIG. 1 shows an example of the optical amplification method of the present invention. In the figure, input light a and pumping light from a pumping light source 2 are combined by an optical combiner 3 or an optical multiplexer. It is manually powered by an optical fiber amplifier 2''51 using an element-doped optical fiber.This optical fiber amplifier l may be an erbium-doped optical fiber or a traveling wave optical amplifier using a semiconductor laser.

この光ファイバ増幅器1では励起光すのエネルギーを吸
収し、そのエネルギーにより入力光aを増幅して出力光
Cを出力する。
This optical fiber amplifier 1 absorbs the energy of the pump light S, uses the energy to amplify the input light a, and outputs the output light C.

本発明では入力光aの一部を光分岐器5において例えば
9対lの割合で分岐する。そのうち90%の光aはその
まま光合流器3に入れ、光合流器3で励起光源2から出
力される励起光すと合流させて光ファイバ増幅器lに入
力する。一方1分岐された10%の光はモニタ光dとし
て励起光源2の入力端光・電気変換部21に入力して電
気信号に変換し1次の割算回路(例えば演算増幅器)2
3に人力される2゜ また、本発明では光ファイバ増幅器lの出力光Cを光分
岐器4において例えば9対lの割合で分岐しく分岐する
比率は入力光aの場合と同じとする)、そのうちの90
%の光Cはそのまま出力し1分岐された10%の光をモ
ニタ光eとして励起光fA2の出力側光・電気変換部2
2に人力して電気信号に変換し、前記割算回路23に入
力される。この割算回路23では大力モニタ光dによる
電気信号と出力モニタ光eによる電気信号との比が求め
られる。即ち、出力モニタ光e/人カモニタ光dの値が
電圧値りとして算出され、次の比較回路(例えば演算増
幅器)24に入力されて、基準電圧発生部25で設定さ
れている基l′!!電圧と比較される。
In the present invention, a part of the input light a is split in the optical splitter 5 at a ratio of, for example, 9:1. 90% of the light a enters the optical combiner 3 as it is, where it is combined with the pumping light output from the pumping light source 2 and input to the optical fiber amplifier l. On the other hand, 10% of the light branched into one branch is input as monitor light d to the input end optical-to-electrical converter 21 of the excitation light source 2, where it is converted into an electrical signal and sent to the primary division circuit (for example, an operational amplifier) 2.
In addition, in the present invention, the ratio at which the output light C of the optical fiber amplifier l is branched in the optical splitter 4 at a ratio of, for example, 9 to l is the same as that for the input light a), 90 of them
% of the light C is output as is, and the 10% light that is branched into one is used as the monitor light e to the output side optical-to-electrical converter 2 of the excitation light fA2.
2, the signal is manually converted into an electrical signal, and the signal is input to the division circuit 23. This dividing circuit 23 calculates the ratio between the electrical signal caused by the high-power monitor light d and the electrical signal caused by the output monitor light e. That is, the value of the output monitor light e/person monitor light d is calculated as a voltage value, is input to the next comparison circuit (for example, an operational amplifier) 24, and is input to the base l'! set by the reference voltage generator 25. ! compared to voltage.

基準電圧発生部25は予め望まれる増幅率(例えば20
倍)に相当する電圧(基準電圧)Aが設定されている。
The reference voltage generator 25 has a predetermined amplification factor (for example, 20
A voltage (reference voltage) A corresponding to

比較された結果が電圧として電気・光変換部(励起光出
力部)15に入力され、その入力端子に応じて励起光す
のパワーが増減され、同励起光すが光合成器3を通して
入力光aと合成され、光ファイバ増幅器lの利得が一定
に調整される。
The comparison result is input as a voltage to the electric/optical converter (pumping light output part) 15, and the power of the pumping light is increased or decreased depending on the input terminal, and the pumping light is converted into input light a through the optical combiner 3. The gain of the optical fiber amplifier l is adjusted to a constant value.

(発明の効果) 本発明の光増幅方法は次のようなりh渠がある。(Effect of the invention) The optical amplification method of the present invention has the following features.

■、光ファイバ増幅器lや励起光源2等の周囲温度が変
化しても、また、入力光レベルが変化しても、それらの
変化に依存せずに光ファイバ増幅231の増幅率が一定
となる。このため安定した出力が得られ、また、入力光
の変化に依存することな(常に一定な利得の光ファイバ
増幅器が要求される測定器分野でも使用可能となる。
(2) Even if the ambient temperature of the optical fiber amplifier 1, the pumping light source 2, etc. changes, or the input light level changes, the amplification factor of the optical fiber amplifier 231 remains constant regardless of these changes. . Therefore, a stable output can be obtained, and it can also be used in the field of measuring instruments, where an optical fiber amplifier with a constant gain that does not depend on changes in input light is required.

■、出出力モニタ光0大 較される基$値を変えることにより光ファイバ増幅器の
増幅率を容易に変えることができる。
(2) The amplification factor of the optical fiber amplifier can be easily changed by changing the base value to which the output output monitor light is compared.

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

第1図は本発明の光増幅方法の説明図、第2図は従来の
光増幅方法の説明図、第3図は本件発明イらが先に開発
した光増幅方法の説明図である。 lは光ファイバ増幅器 aは入力光 すは励起光 Cは出向先 dは人力モニタ光 eは出力モニタ光
FIG. 1 is an explanatory diagram of the optical amplification method of the present invention, FIG. 2 is an explanatory diagram of the conventional optical amplification method, and FIG. 3 is an explanatory diagram of the optical amplification method previously developed by the present inventors. l is the optical fiber amplifier a is the input light, pump light C is the destination d is the human power monitor light e is the output monitor light

Claims (1)

【特許請求の範囲】[Claims] 入力光aと励起光bとを合成して光ファイバ増幅器1に
入力し、前記入力光aを同増幅器1により増幅して出力
光cとするようにした光増幅方法において、前記入力光
aの一部を取り出して入力モニタ光dとし、前記出力光
cの一部を取り出して出力モニタ光eとし、両モニタ光
d、eのレベル比を予め設定されている基準値と比較し
て、同レベル比が基準値と一致するように励起光bの出
力パワーを自動調整するようにしたことを特徴とする光
増幅方法。
In an optical amplification method, input light a and pump light b are combined and input to an optical fiber amplifier 1, and the input light a is amplified by the same amplifier 1 to produce an output light c. A part of the output light c is taken out as the input monitor light d, a part of the output light c is taken out as the output monitor light e, and the level ratio of both monitor lights d and e is compared with a preset reference value. An optical amplification method characterized in that the output power of pumping light b is automatically adjusted so that the level ratio matches a reference value.
JP1128961A 1989-05-24 1989-05-24 Light amplification Pending JPH02308581A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1128961A JPH02308581A (en) 1989-05-24 1989-05-24 Light amplification

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1128961A JPH02308581A (en) 1989-05-24 1989-05-24 Light amplification

Publications (1)

Publication Number Publication Date
JPH02308581A true JPH02308581A (en) 1990-12-21

Family

ID=14997696

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1128961A Pending JPH02308581A (en) 1989-05-24 1989-05-24 Light amplification

Country Status (1)

Country Link
JP (1) JPH02308581A (en)

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04251827A (en) * 1991-01-29 1992-09-08 Nec Corp Optical amplification system and device
JPH0521881A (en) * 1991-07-17 1993-01-29 Nec Corp Optical fiber amplifier
JPH0537066A (en) * 1991-08-01 1993-02-12 Nec Corp Light repeater
EP0871302A2 (en) * 1997-03-28 1998-10-14 Lucent Technologies Inc. Dynamic gain control system for optical amplifier and method thereof
EP1283567A2 (en) * 2001-07-10 2003-02-12 Samsung Electronics Co., Ltd. Automatic gain control device of optical fiber amplifier
EP1394970A3 (en) * 2002-08-30 2006-01-11 Sumitomo Electric Industries, Ltd. Optical amplifier, gain control method and circuit for an optical amplifier
CN1318909C (en) * 2002-08-30 2007-05-30 住友电气工业株式会社 Light amplifier, gain-control method for light amplifier and electric circuit
US7538937B2 (en) 2002-03-14 2009-05-26 Nippon Telegraph And Telephone Optical amplifier

Cited By (12)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04251827A (en) * 1991-01-29 1992-09-08 Nec Corp Optical amplification system and device
JPH0521881A (en) * 1991-07-17 1993-01-29 Nec Corp Optical fiber amplifier
JPH0537066A (en) * 1991-08-01 1993-02-12 Nec Corp Light repeater
EP0871302A2 (en) * 1997-03-28 1998-10-14 Lucent Technologies Inc. Dynamic gain control system for optical amplifier and method thereof
EP0871302A3 (en) * 1997-03-28 1998-11-25 Lucent Technologies Inc. Dynamic gain control system for optical amplifier and method thereof
US5923462A (en) * 1997-03-28 1999-07-13 Lucent Technologies Inc. Dynamic gain control system for optical amplifier and method thereof
EP1283567A2 (en) * 2001-07-10 2003-02-12 Samsung Electronics Co., Ltd. Automatic gain control device of optical fiber amplifier
EP1283567A3 (en) * 2001-07-10 2003-12-17 Samsung Electronics Co., Ltd. Automatic gain control device of optical fiber amplifier
US7538937B2 (en) 2002-03-14 2009-05-26 Nippon Telegraph And Telephone Optical amplifier
US7589888B2 (en) 2002-03-14 2009-09-15 Nippon Telegraph And Telephone Corporation Optical amplifier having a constant gain profile
EP1394970A3 (en) * 2002-08-30 2006-01-11 Sumitomo Electric Industries, Ltd. Optical amplifier, gain control method and circuit for an optical amplifier
CN1318909C (en) * 2002-08-30 2007-05-30 住友电气工业株式会社 Light amplifier, gain-control method for light amplifier and electric circuit

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