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JPS6364035A - Light wavelength converting circuit - Google Patents

Light wavelength converting circuit

Info

Publication number
JPS6364035A
JPS6364035A JP61209008A JP20900886A JPS6364035A JP S6364035 A JPS6364035 A JP S6364035A JP 61209008 A JP61209008 A JP 61209008A JP 20900886 A JP20900886 A JP 20900886A JP S6364035 A JPS6364035 A JP S6364035A
Authority
JP
Japan
Prior art keywords
light
face
wavelength
incident
emitted
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
JP61209008A
Other languages
Japanese (ja)
Inventor
Shuji Suzuki
修司 鈴木
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
NEC Corp
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 NEC Corp filed Critical NEC Corp
Priority to JP61209008A priority Critical patent/JPS6364035A/en
Priority to DE3689583T priority patent/DE3689583T2/en
Priority to CA000523515A priority patent/CA1274612A/en
Priority to EP86116132A priority patent/EP0223258B1/en
Priority to US06/934,573 priority patent/US4845703A/en
Publication of JPS6364035A publication Critical patent/JPS6364035A/en
Pending legal-status Critical Current

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  • Optical Communication System (AREA)

Abstract

PURPOSE:To contrive a simplified constitution by making the modulated light having a second wavelength incident on a nonlinear optical element having a differential gain characteristic and modulating it with an optical signal having a first wavelength and using a light wavelength filter to take out only the light having the second wavelength of the output light. CONSTITUTION:The signal light having a wavelength lambda1 which is made incident on an end face 104 of a light wavelength filter 102 is emitted from an end face 106 and is made incident on an end face 107 of a nonlinear optical element 101. The modulated light having a wavelength lambda2 which is made incident on an end face 105 of the filter 102 is emitted from the end face 106 and is made incident on the end face 107 of the element 101. The light emitted from an end face 108 of the element 101 is made incident on an end face 109 of a light wavelength filter 103, and only the component having the wavelength lambda2 is emitted from the end face 101. Thus, the constitution is simplified and the light wavelength is converted on the level of light.

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は波長分割光交換機等で使用される光波長変換回
路に関する。
DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to an optical wavelength conversion circuit used in a wavelength division optical exchange or the like.

(従来の技術) 伝送路に光ファイバを用いた光フアイバ伝送方式は、光
ファイバが広帯域であることから多量の情報を伝送可能
であることや、光ファイバが誘導雑音を受けない等の利
点があることから、今後広く使用されるものと予想され
る。この光フアイバ伝送方式とともに交換機には、光信
号を光の領域で交換できる光交換機が望ましい。そのよ
うな光交換機として、特許57−079388号明細書
記載の波長分割光交換機が知られている。波長分割光交
換機では波長多重された入・出力光信号の各波長間に通
話チャンネルを設定し波長を変換することによって交換
を行なう、したがって光信号の波長を変換する光波長変
換回路が必要不可欠である。従来の波長変換回路は第5
図に示すように、波長λ1の入力信号光を受光素子50
1で電気信号に変換し、その電気信号を電気アンプ50
2で増幅した後に出力波長がλ2である発光素子503
を駆動する事によって波長λ2へ波長変換して出力する
構成となっていた。
(Prior art) Optical fiber transmission systems that use optical fibers as transmission paths have the advantages of being able to transmit a large amount of information because the optical fiber has a wide band, and that the optical fiber is not subject to induced noise. Therefore, it is expected that it will be widely used in the future. In addition to this optical fiber transmission system, it is desirable to use an optical switch that can exchange optical signals in the optical domain. As such an optical exchanger, a wavelength division optical exchanger described in Japanese Patent No. 57-079388 is known. In a wavelength-division optical switch, a communication channel is established between each wavelength of wavelength-multiplexed input and output optical signals, and switching is performed by converting the wavelengths. Therefore, an optical wavelength conversion circuit that converts the wavelength of the optical signal is essential. be. The conventional wavelength conversion circuit is the fifth
As shown in the figure, the input signal light of wavelength λ1 is sent to the light receiving element 50.
1 converts the electrical signal into an electrical signal, and converts the electrical signal into an electrical amplifier 50.
A light emitting element 503 whose output wavelength is λ2 after being amplified by 2
By driving the wavelength λ2, the wavelength is converted to λ2 and outputted.

(発明が解決しようとする問題点) このような波長変換回路は現状では以下の理由により集
積化が難かしく規模が大きくなる上に低コスト化が難か
しいという問題がある。すなわち、発光素子、受光素子
はInP系の材料を用いて作られているが、これに対し
電気アンプなどの電気回路はSi、 GaAs系の材料
が用いられているため、光波長変換回路は、複雑な構成
とならざるをえない、電気回路を InP系の材料で作
れば構成を簡単にすることはできるが、現状の技術では
InP系の材料で電気回路を高集積化するのは難かしい
(Problems to be Solved by the Invention) Currently, such wavelength conversion circuits have problems in that they are difficult to integrate, increase in scale, and are difficult to reduce cost due to the following reasons. In other words, light emitting elements and light receiving elements are made using InP-based materials, whereas electrical circuits such as electric amplifiers are made from Si or GaAs-based materials. Although it is possible to simplify the configuration of electrical circuits, which are inevitably complicated, by making them using InP-based materials, it is difficult to achieve high integration of electrical circuits using InP-based materials with current technology. .

本発明は、簡単な構成を有し光波長変換回路を提供する
ことを目的とする。
An object of the present invention is to provide an optical wavelength conversion circuit having a simple configuration.

(問題を解決するための手段) 本発明の提供する光波長変換回路は入射光量と透過率と
の関係に微分利得特性を有し、変調された第1の波長の
信号光および第2の波長の被変調光が入力された非線形
光学素子と、前記非線形光学素子の出力光から前記第2
の波長の光選択して取り出す光波長フィルタを少なくと
も含むことを特徴とする。
(Means for Solving the Problem) The optical wavelength conversion circuit provided by the present invention has a differential gain characteristic in the relationship between the amount of incident light and the transmittance, and has a differential gain characteristic in the relationship between the amount of incident light and the transmittance. a nonlinear optical element into which the modulated light of
The device is characterized in that it includes at least an optical wavelength filter that selectively extracts light having a wavelength of .

さらに本発明の提供する光波長変換回路は複数の端面を
有し第1の端面と第1の波長の被変調光が入力され前記
第1の端面と第2の端面の入射光量と透過率との関係に
微分利得特性を有する非線形光学素子と、第1の端面へ
の入射光は第2の端面から出射されるが第3の端面から
は出射されず前記第2の端面への入射光は前記第3の端
面から出射され前記第1の端面に第2の波長の信号光が
入射され前記第2の端面が前記非線形光学素子の前記第
2の端面に接している方向性光学素子とを少なくとも含
む事を特徴とする。
Furthermore, the optical wavelength conversion circuit provided by the present invention has a plurality of end faces, and modulated light of a first wavelength is inputted to the first end face, and the incident light amount and transmittance of the first end face and the second end face are determined. A nonlinear optical element having a differential gain characteristic in the relationship: the light incident on the first end face is emitted from the second end face but not the third end face, and the light incident on the second end face is emitted from the second end face. a directional optical element in which signal light of a second wavelength is emitted from the third end face and is incident on the first end face, and the second end face is in contact with the second end face of the nonlinear optical element; It is characterized by containing at least

(作用) 本発明では、このように微分利得特性を有する非線形光
学素子に第2の波長の被変調光を入力し、第1の波長の
光信号で変調し、出力光の白菜2の波長の光のみを光波
長フィルタまたは光合流器を用いて取り出す。
(Function) In the present invention, the modulated light of the second wavelength is input to the nonlinear optical element having differential gain characteristics as described above, and is modulated by the optical signal of the first wavelength, so that the output light has the wavelength of Chinese cabbage 2. Only light is extracted using an optical wavelength filter or optical combiner.

したがって構成が簡単で、光波長を直接変換する波長変
換回路を本発明により得ることができる。
Therefore, the present invention can provide a wavelength conversion circuit that has a simple configuration and directly converts optical wavelengths.

(実施例) 以下本発明の実施例について図面を参照して説明する。(Example) Embodiments of the present invention will be described below with reference to the drawings.

第1図は本発明の第1の実施例を示す図である。第1図
において、光波長フィルタ102の端面104へ入射さ
れた波長λ1の信号光は端面106から出射され非線形
光学素子101の端面107へ入射される。光波長フィ
ルタ102の端面105へ入射された波長λ2の被変調
光は、やはり端面106から出射され非線形光学素子1
01の端面107へ入射される。非線形光学素子101
の端面10Bからの出射光は光波長フィルタ103の端
面109へ入射され、波長λ2の成分のみ端面110か
ら出射される。
FIG. 1 is a diagram showing a first embodiment of the present invention. In FIG. 1, a signal light having a wavelength λ1 that is incident on the end face 104 of the optical wavelength filter 102 is emitted from the end face 106 and is made incident on the end face 107 of the nonlinear optical element 101. The modulated light of wavelength λ2 incident on the end face 105 of the optical wavelength filter 102 is also emitted from the end face 106 and passes through the nonlinear optical element 1.
The light is incident on the end face 107 of 01. Nonlinear optical element 101
The light emitted from the end face 10B is incident on the end face 109 of the optical wavelength filter 103, and only the component of wavelength λ2 is emitted from the end face 110.

第2図は、第1図の本発明の第1の実施例の動作を説明
する為の図であり、非線形光学素子101の入射光量と
透過率との関係を表わしている。非線形光学素子101
は入力光量がOでは透過率もOで、入力光量を増加させ
P2を越えると透過率が0から1.まで急激に増加する
微分利得特性を有している。第1図における非線形光学
素子101の端面107へ入射される光の内、波長λ2
の被変調光の成分の光量をP2より小さいP、に設定し
ておき、波長λlの信号光の成分の光量を低レベルでは
0、高レベルではP、としてP、+P、がP2より大き
いように設定しておく、すると波長λ1の信号光が低レ
ベルであれば非線形光学素子101の入力光量はPlで
あるので出力光量はO1高レベルであれば入力光量はP
、+P、>P2であるので透過率はtlで出力光量はt
、(P、+P3)となるので波長^1の信号光の2値の
レベルに応じて出力光量のレベルも変化する。したがっ
て端面108からの出力光の内、波長λ2の成分を光波
長フィルタ103によって選択すれば、波長がλ2で波
長λlと同じ2値レベルの情報を有する変調光が得られ
波長^lからλ2への波長変換を行なうことが出来る。
FIG. 2 is a diagram for explaining the operation of the first embodiment of the present invention shown in FIG. 1, and shows the relationship between the amount of incident light and the transmittance of the nonlinear optical element 101. Nonlinear optical element 101
When the input light amount is O, the transmittance is also O, and when the input light amount is increased and exceeds P2, the transmittance changes from 0 to 1. It has a differential gain characteristic that rapidly increases up to . Of the light incident on the end face 107 of the nonlinear optical element 101 in FIG.
The light intensity of the modulated light component is set to P, which is smaller than P2, and the light intensity of the signal light component with wavelength λl is set to 0 at low level and P at high level, so that P, +P, is larger than P2. If the signal light with wavelength λ1 is at a low level, the input light amount of the nonlinear optical element 101 is Pl, so the output light amount is O1.If the signal light is at a high level, the input light amount is P.
, +P, >P2, so the transmittance is tl and the output light amount is t
, (P, +P3), so the level of the output light quantity also changes according to the binary level of the signal light of wavelength ^1. Therefore, if the wavelength λ2 component of the output light from the end face 108 is selected by the optical wavelength filter 103, modulated light having the wavelength λ2 and the same binary level information as the wavelength λl can be obtained, and from the wavelength ^l to the wavelength λ2. wavelength conversion can be performed.

なお微分利得特性を有する非線形光学素子101として
は、多重量子井戸構造素子の吸収特性の入力光による変
化を利用したもの、光共振器内の屈折率の入力光による
変化を利用したもの等、様々な原理にもとすく素子が存
在する。多重量子井戸構造素子の吸収特性の入力光によ
る変化については、例えばアイ・イー・イー・イー、ジ
ャーナル・オブ・カンタム・エレクトロニクス(IEE
EJournal of Quanturn Elec
tronics) 20巻 3号 265ページから2
75ページに、光共振器内の屈折率の入力光による変化
についてはアプライド・フィジックス・レターく^pp
lied Physics Letter)46(10
)巻1985年5月15日号918ページから 920
ページに詳細に記述されている。
There are various types of nonlinear optical element 101 having differential gain characteristics, such as one that utilizes a change in absorption characteristics of a multi-quantum well structure element due to input light, and one that utilizes a change in refractive index within an optical resonator due to input light. There are many elements based on this principle. Regarding changes in absorption characteristics of multi-quantum well structure elements depending on input light, see, for example, IEE, Journal of Quantum Electronics (IEE).
EJournal of Quantum Elec
tronics) Volume 20, Issue 3, Pages 265-2
On page 75, there is an Applied Physics Letter regarding changes in the refractive index within an optical cavity due to input light.
Lied Physics Letter) 46 (10
) volume May 15, 1985 issue pages 918 to 920
detailed on the page.

第3図は本発明の第2の実施例を示す図であり、第1図
と同じ番号を附したものは、第1図と同一の構成要素を
表わす。第3図において光波長フィルタ301の端面3
02に入射された波長λlの光信号は端面303から出
射され非線形光学素子101の端面107へ入射される
。一方、非線形光学素子101の端面108へは波長λ
2の被変調光が入射されている。ここで波長^2の被変
調光の光量を第2図に示すP2、端面107へ入射する
波長λlの信号光の低レベルの光量は0、高レベルの光
量をP、に設定すれば非線形光学素子101の透過率は
端面107,10Bへの入射光量の和に応じてOから1
゜まで変化する。よって端面108から入射され、端面
107から出射される波長λ2の光は波長λ、の信号光
の2値レベルに応じた透過率の変化により変調される。
FIG. 3 is a diagram showing a second embodiment of the present invention, and the same numbers as in FIG. 1 represent the same components as in FIG. 1. In FIG. 3, the end face 3 of the optical wavelength filter 301
The optical signal having the wavelength λl incident on the nonlinear optical element 101 is emitted from the end face 303 and is incident on the end face 107 of the nonlinear optical element 101. On the other hand, the wavelength λ
Two modulated lights are incident. Here, if the light intensity of the modulated light of wavelength ^2 is set to P2 shown in FIG. The transmittance of the element 101 varies from O to 1 depending on the sum of the amounts of light incident on the end surfaces 107 and 10B.
It changes up to ゜. Therefore, the light having the wavelength λ2 that is incident from the end face 108 and emitted from the end face 107 is modulated by a change in transmittance according to the binary level of the signal light having the wavelength λ.

この波長λ2の変調光は端面303へ入射された光から
波長λ2の光のみと端面304から出射する光波長フィ
ルタ301によって分離することが出来る。
This modulated light of wavelength λ2 can be separated from the light incident on the end face 303 by the light wavelength filter 301 that outputs only the light of wavelength λ2 from the end face 304.

第4図は本発明の第3の実施例を示す図であり、第1図
と同じ番号を附したものは第3図と同一の構成要素を表
わし光波長301に替えて光合流器402を使用してい
る点以外は同じ構成である。
FIG. 4 is a diagram showing a third embodiment of the present invention, in which the same numbers as in FIG. 1 represent the same components as in FIG. The configuration is the same except for the one used.

第4図において波長^、の信号光は光合流器402経由
で非線形光学素子101の端面107へ入射され、波長
λ2の被変調光は端面10Bへ入射されている。ここで
波長λ2の被変調光の光量をやはり第2図に示すP2に
、端面107へ入射する波長λ1の信号光の低レベルの
光量はO1高レベルの光量をP3に設定すれば端面10
日から入射され端面187から出射される波長λ2の光
は波長λ、の信号光の2値レベルに応じて変調される。
In FIG. 4, the signal light with wavelength ^ is input to the end face 107 of the nonlinear optical element 101 via the optical combiner 402, and the modulated light with the wavelength λ2 is input to the end face 10B. Here, if the light intensity of the modulated light of wavelength λ2 is set to P2 shown in FIG.
The light of wavelength λ2 which enters from the sun and is emitted from the end face 187 is modulated according to the binary level of the signal light of wavelength λ.

この波長λ2の変調光は光合流402の端面406へ入
射され端面405から取り出す事が出来る。
This modulated light of wavelength λ2 is incident on the end face 406 of the light confluencer 402 and can be taken out from the end face 405.

なお光合流器402のかわりに、端面404への入射光
は端面406から出射するのが端面405からは出射せ
ず、端面406への入射光は端面405から出射する光
サーキュレータ等を用いても同様の効果を得る事が出来
る。
Note that instead of the light combiner 402, an optical circulator or the like may be used in which the light incident on the end face 404 is emitted from the end face 406 but not from the end face 405, and the light incident on the end face 406 is emitted from the end face 405. A similar effect can be obtained.

(発明の効果) このように本発明によれば、構成が簡単で、光波長を光
のレベルで変換することができる光波長変換回路を得る
ことが出来る。
(Effects of the Invention) As described above, according to the present invention, it is possible to obtain an optical wavelength conversion circuit that has a simple configuration and is capable of converting optical wavelengths at the optical level.

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

第1図は本発明の第1の実施例を示す図、第2図は第1
図の本発明の第1の実施例の動作を説明する為の図、第
3図は本発明の第2の実施例を示す図、第4図は本発明
の第3の実施例を示す図、第5図は従来の光波長変換回
路の構成を示す図である。 図において101は非線形光学素子を、102.103
.301は光波長フィルタを、402は光合流器を、5
01は受光素子を、502は電気アンプを、503は発
光素子を各々表わす。 第2図 !!!!!     禮
FIG. 1 is a diagram showing a first embodiment of the present invention, and FIG. 2 is a diagram showing a first embodiment of the present invention.
3 is a diagram showing the second embodiment of the present invention, and FIG. 4 is a diagram showing the third embodiment of the present invention. , FIG. 5 is a diagram showing the configuration of a conventional optical wavelength conversion circuit. In the figure, 101 is a nonlinear optical element, 102.103
.. 301 is an optical wavelength filter, 402 is an optical combiner, 5
01 represents a light receiving element, 502 represents an electric amplifier, and 503 represents a light emitting element. Figure 2! ! ! ! ! grace

Claims (2)

【特許請求の範囲】[Claims] (1)入射光量と透過率との関係に微分利得特性を有し
、変調された第1の波長の信号光および第2の波長の被
変調光が入力された非線形光学素子と、前記非線形光学
素子の出力光から前記第2の波長の光選択して取り出す
光波長フィルタを少なくとも含むことを特徴とする光波
長変換回路。
(1) A nonlinear optical element having a differential gain characteristic in the relationship between the amount of incident light and the transmittance, into which modulated signal light of a first wavelength and modulated light of a second wavelength are input; An optical wavelength conversion circuit comprising at least an optical wavelength filter that selects and extracts light of the second wavelength from the output light of the element.
(2)複数の端面を有し第1の端面と第1の波長の被変
調光が入力され前記第1の端面と第2の端面の入射光量
と透過率との関係に微分利得特性を有する非線形光学素
子と、第1の端面への入射光は第2の端面から出射され
るが第3の端面からは出射されず前記第2の端面への入
射光は前記第3の端面から出射され前記第1の端面に第
2の波長の信号光が入射され前記第2の端面が前記非線
形光学素子の前記第2の端面と接している方向性光学素
子とを少なくとも含むことを特徴とする光波長変換回路
(2) It has a plurality of end faces, and modulated light of a first wavelength is input to the first end face, and the relationship between the amount of incident light and the transmittance of the first end face and the second end face has a differential gain characteristic. A nonlinear optical element, in which light incident on the first end face is emitted from the second end face but not emitted from the third end face, and light incident on the second end face is emitted from the third end face. A light comprising at least a directional optical element in which a signal light of a second wavelength is incident on the first end face, and the second end face is in contact with the second end face of the nonlinear optical element. Wavelength conversion circuit.
JP61209008A 1985-11-22 1986-09-04 Light wavelength converting circuit Pending JPS6364035A (en)

Priority Applications (5)

Application Number Priority Date Filing Date Title
JP61209008A JPS6364035A (en) 1986-09-04 1986-09-04 Light wavelength converting circuit
DE3689583T DE3689583T2 (en) 1985-11-22 1986-11-21 Optical wavelength division multiplex switching system with wavelength switching light modulators.
CA000523515A CA1274612A (en) 1985-11-22 1986-11-21 Wavelength division optical switching system having wavelength switching light modulators
EP86116132A EP0223258B1 (en) 1985-11-22 1986-11-21 Wavelength division optical switching system having wavelength switching light modulators
US06/934,573 US4845703A (en) 1985-11-22 1986-11-24 Wavelength division optical switching system having wavelength switching light modulators

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61209008A JPS6364035A (en) 1986-09-04 1986-09-04 Light wavelength converting circuit

Publications (1)

Publication Number Publication Date
JPS6364035A true JPS6364035A (en) 1988-03-22

Family

ID=16565758

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61209008A Pending JPS6364035A (en) 1985-11-22 1986-09-04 Light wavelength converting circuit

Country Status (1)

Country Link
JP (1) JPS6364035A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02502150A (en) * 1987-11-20 1990-07-12 ブリテツシユ・テレコミユニケイシヨンズ・パブリツク・リミテツド・カンパニー optical switching network

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6195322A (en) * 1984-10-17 1986-05-14 Nec Corp Device for generating phase modulating light for optical communication

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6195322A (en) * 1984-10-17 1986-05-14 Nec Corp Device for generating phase modulating light for optical communication

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02502150A (en) * 1987-11-20 1990-07-12 ブリテツシユ・テレコミユニケイシヨンズ・パブリツク・リミテツド・カンパニー optical switching network

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