JP2002016308A - Polarized light source device - Google Patents

Polarized light source device

Info

Publication number
JP2002016308A
JP2002016308A JP2000193677A JP2000193677A JP2002016308A JP 2002016308 A JP2002016308 A JP 2002016308A JP 2000193677 A JP2000193677 A JP 2000193677A JP 2000193677 A JP2000193677 A JP 2000193677A JP 2002016308 A JP2002016308 A JP 2002016308A
Authority
JP
Japan
Prior art keywords
polarized light
light source
source device
light sources
linearly polarized
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
JP2000193677A
Other languages
Japanese (ja)
Inventor
Yoshikazu Toba
良和 鳥羽
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.)
Tokin Corp
Original Assignee
Tokin 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 Tokin Corp filed Critical Tokin Corp
Priority to JP2000193677A priority Critical patent/JP2002016308A/en
Publication of JP2002016308A publication Critical patent/JP2002016308A/en
Pending legal-status Critical Current

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  • Optical Couplings Of Light Guides (AREA)
  • Lasers (AREA)

Abstract

PROBLEM TO BE SOLVED: To provide two linear polarized light sources wherein beat noise frequency due to interference between output lights can be controlled. SOLUTION: This polarized light source is provided with two light sources outputting linear polarized lights, and a photocoupler which synthesizes the linear polarized lights in such a manner that polarization surfaces of the linear polarized lights are made perpendicular to each other. An optical attenuator is so arranged that intensity of an output light of at least one out of the two light sources is attenuated.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明は、偏光を制御したレ
ーザ光源に係り、特に、波長がわずかに異なり、偏波面
が互いに垂直な、二つの直線偏光を出射する半導体レー
ザ励起固体レーザ光源に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a laser light source whose polarization is controlled, and more particularly to a semiconductor laser-excited solid-state laser light source which emits two linearly polarized lights having slightly different wavelengths and mutually perpendicular polarization planes.

【0002】[0002]

【従来の技術】一般に、光通信及び光計測分野において
用いられる光デバイスの多くは偏波依存性があるため
に、光ファイバには伝送距離に関わらず、偏波保持ファ
イバを使用することが好ましい。
2. Description of the Related Art In general, most optical devices used in the field of optical communication and optical measurement have polarization dependence. Therefore, it is preferable to use a polarization maintaining fiber for an optical fiber regardless of the transmission distance. .

【0003】しかしながら、少なくとも現状において
は、偏波保持ファイバの価格はシングルモードファイバ
の価格の10倍程度であり、特に遠隔伝送が必要な伝送
システムにおいては、システム全体のうち、伝送路が占
めるコストは、当該システムの存在自体を脅かすといっ
ても過言ではない。
However, at least at present, the cost of a polarization maintaining fiber is about ten times the price of a single mode fiber, and especially in a transmission system that requires remote transmission, the cost occupied by the transmission line in the entire system. It is no exaggeration to say that it threatens the existence of the system itself.

【0004】他方、シングルモードファイバを伝送路と
した場合、ここでの偏波面の変動は回避できないため、
受光側において、一定の偏光方向で一定の光強度を得る
ためには、偏光面が直交する二つの直線偏光光源が必要
とされる。
On the other hand, when a single-mode fiber is used as the transmission line, fluctuations in the polarization plane cannot be avoided here.
In order to obtain a constant light intensity in a constant polarization direction on the light receiving side, two linearly polarized light sources whose polarization planes are orthogonal to each other are required.

【0005】このような背景のもとに、経済性追求の必
要から、光伝送路として、偏波保持ファイバに代わっ
て、シングルモードファイバを用いることによる動作上
の不利を補う方法が検討されてきた。
[0005] Against this background, there is a need to pursue economic efficiency, and a method for compensating for the operation disadvantage caused by using a single-mode fiber instead of a polarization-maintaining fiber as an optical transmission line has been studied. Was.

【0006】その一つとして、従来において、図2に示
すような光源が用いられている(以下、従来技術と呼
ぶ)。図2に示すように、光源は二つの直線偏光光源2
1,22と光結合器26とを各々接続する偏波保持ファ
イバ24,25とを備え、光結合器26からの光は、シ
ングルモードファイバ27によって導き出されている。
図2において、横方向の矢印は水平方向の偏波面を備え
た光を、縦方向の矢印は垂直方向の偏波面を備えた光を
それぞれ示している。
As one of them, a light source as shown in FIG. 2 has been conventionally used (hereinafter, referred to as conventional technology). As shown in FIG. 2, the light sources are two linearly polarized light sources 2.
Polarization maintaining fibers 24 and 25 are provided to connect the optical couplers 1 and 22 and the optical coupler 26, respectively, and light from the optical coupler 26 is guided by a single mode fiber 27.
In FIG. 2, a horizontal arrow indicates light having a horizontal polarization plane, and a vertical arrow indicates light having a vertical polarization plane.

【0007】このような構成の従来技術による光源にお
いて、2つの直線偏光光源21,22から出射される直
線偏光は光結合器26で偏波面が互いに直交するように
合成され、長いシングルモードファイバ27の他端に接
続される光デバイスの直前に検光子を付加すれば、実質
的に偏波保持ファイバを用いたときと同等の効果が得ら
れる。
In the light source according to the prior art having such a configuration, the linearly polarized lights emitted from the two linearly polarized light sources 21 and 22 are combined by the optical coupler 26 so that the polarization planes are orthogonal to each other. If an analyzer is added immediately before the optical device connected to the other end of the optical fiber, an effect substantially equivalent to the case where a polarization maintaining fiber is used can be obtained.

【0008】図3は、図2に示された二直線偏光光源を
構成する一方の半導体レーザ励起固体レーザ光源から成
る直線偏光光源21又は22の概略構成を示す図であ
る。励起用の半導体レーザ8、凸レンズである第1の光
学レンズ9、光共振器14、凸レンズである第2の光学
レンズ13、及び偏波面保持ファイバ24又は25が、
順に設けられている。
FIG. 3 is a diagram showing a schematic configuration of a linearly polarized light source 21 or 22 composed of one semiconductor laser-excited solid-state laser light source constituting the bilinearly polarized light source shown in FIG. The semiconductor laser 8 for excitation, the first optical lens 9 as a convex lens, the optical resonator 14, the second optical lens 13 as a convex lens, and the polarization plane holding fiber 24 or 25 include:
They are provided in order.

【0009】光共振器14は、それぞれ凹面を備えた一
対のミラー10,12の間にレーザ媒質11である固体
レーザ用結晶が挿入されて構成されている。即ち、この
光源は、半導体レーザ8の励起光によって、光共振器1
4内でレーザ発振がなされる。
The optical resonator 14 is constructed by inserting a solid-state laser crystal as the laser medium 11 between a pair of mirrors 10 and 12 each having a concave surface. That is, this light source is driven by the excitation light of the
In 4, laser oscillation is performed.

【0010】尚、ここでの直線偏光光源21,22、及
び光結合器26と、これらの間を結合した一対の偏波保
持ファイバ24,25とは出射光を二つの直線偏光の偏
波面が垂直をなすように合成して出射するので、合わせ
て偏光光源装置と呼ばれてもよい。
Here, the linearly polarized light sources 21 and 22 and the optical coupler 26 and the pair of polarization maintaining fibers 24 and 25 coupled between them are used to convert the outgoing light into two linearly polarized light planes. Since the light is synthesized and emitted so as to be vertical, it may be collectively called a polarized light source device.

【0011】[0011]

【発明が解決しようとする課題】しかしながら、従来技
術による光源の場合、レーザ媒質の組成、厚みばらつき
により、二つの光源の各々の出射光波長の制御が困難で
あり、出射光間で干渉が生じる場合があった。加えて干
渉によるビートノイズの周波数を制御することが困難で
あった。
However, in the case of the light source according to the prior art, it is difficult to control the wavelength of the emitted light of each of the two light sources due to variations in the composition and thickness of the laser medium, and interference occurs between the emitted light. There was a case. In addition, it has been difficult to control the frequency of beat noise due to interference.

【0012】そこで、本発明の課題は、従来技術による
二直線偏光光源における前述の問題点を解決し、出射光
間での干渉によるビートノイズ周波数の制御可能な二直
線偏光光源を提供することにある。
An object of the present invention is to solve the above-mentioned problems in the conventional linearly polarized light source and to provide a linearly polarized light source capable of controlling the beat noise frequency due to interference between the emitted lights. is there.

【0013】[0013]

【課題を解決するための手段】前記課題を解決するため
に、本発明の偏光光源装置は、直線偏光を出射する二つ
の光源と、これらの光源から出射する二つ直線偏光を偏
波面が互いに垂直になるように合成する光結合器とを備
えた偏光光源装置であって、前記二つの光源のうち少な
くとも一方は光の減衰機構を備えることを特徴とする。
In order to solve the above-mentioned problems, a polarized light source device according to the present invention comprises two light sources for emitting linearly polarized light and two linearly polarized light beams emitted from these light sources. A polarized light source device comprising: an optical coupler for vertically combining light, wherein at least one of the two light sources includes a light attenuation mechanism.

【0014】また、前記二つの光源は半導体レーザ励起
固体レーザとすることができる。
Further, the two light sources may be solid-state lasers excited by a semiconductor laser.

【0015】また、前記二つの光源における励起用半導
体レーザの駆動電流の値を異なるように設定した場合に
も、前記光結合器から出射する、偏波面が互いに垂直な
二つの直線偏光の強度が等しくなるように、前記減衰機
構の減衰量が設定できるようにすると良い。
Further, even when the values of the drive currents of the pumping semiconductor lasers in the two light sources are set to be different from each other, the intensities of the two linearly polarized light beams having mutually perpendicular polarization planes emitted from the optical coupler are different from each other. It is preferable that the damping amount of the damping mechanism can be set to be equal.

【0016】[0016]

【発明の実施の形態】以下に本発明の実施の形態につい
て、図面を参照して説明する。
Embodiments of the present invention will be described below with reference to the drawings.

【0017】図1は、本発明の一実施形態に係る偏光光
源装置の基本構成を示す。この偏光光源装置は、互いに
垂直な直線偏光を出射する二つの直線偏光光源1,2
と、これらの直線偏光光源1,2からの二つの直線偏光
を、偏波面が互いに垂直な状態で合成する光結合器6と
を備え、直線偏光光源1及び光結合器6を光減衰器3
(減衰量0.5dB)を介して、比較的短い偏波保持フ
ァイバ4で結合され、一方、直線偏光光源2及び光結合
器6は光減衰器を介さないで、比較的短い偏波保持ファ
イバ5で結合されている。なお、二つの直線偏光光源
1,2の構成は、半導体レーザ励起固体レーザであっ
て、従来例として、図3を用いて説明したものと同様で
ある。
FIG. 1 shows a basic configuration of a polarized light source device according to an embodiment of the present invention. This polarized light source device comprises two linearly polarized light sources 1 and 2 that emit linearly polarized light perpendicular to each other.
And an optical coupler 6 for combining the two linearly polarized lights from the linearly polarized light sources 1 and 2 with their polarization planes perpendicular to each other.
(Attenuation: 0.5 dB), and are coupled by a relatively short polarization maintaining fiber 4, while the linearly polarized light source 2 and the optical coupler 6 are relatively short polarization maintaining fibers without an optical attenuator. 5 are connected. The configuration of the two linearly polarized light sources 1 and 2 is a semiconductor laser pumped solid-state laser, and is the same as that described with reference to FIG. 3 as a conventional example.

【0018】この偏光光源装置において、光結合器6か
ら出射する各々の偏光軸の強度比、即ち互いに垂直な偏
波面を有する二つの偏光の間の強度比を半導体レーザの
駆動電流によって等しくなるように調整した。
In this polarized light source device, the intensity ratio of each polarization axis emitted from the optical coupler 6, that is, the intensity ratio between two polarized lights having polarization planes perpendicular to each other, is made equal by the driving current of the semiconductor laser. Was adjusted.

【0019】本実施の形態により作製した半導体レーザ
励起固体レーザ光源に、1kmのシングルモード光ファ
イバを接続し、光出力部に検光子を付加し、ファイバ伝
送中の偏光変動に対する光出力変動を測定したところ、
0.5dB以下であり、実質的に偏波保持ファイバを用
いたのと同等の効果が得られた。この時の出射光間での
干渉によるビートノイズ周波数は1.6GHzとなっ
た。
A single-mode optical fiber of 1 km is connected to the semiconductor laser-excited solid-state laser light source manufactured according to the present embodiment, an analyzer is added to an optical output unit, and the optical output fluctuation with respect to the polarization fluctuation during fiber transmission is measured. After doing
0.5 dB or less, and an effect substantially equivalent to the use of the polarization maintaining fiber was obtained. The beat noise frequency due to the interference between the emitted lights at this time was 1.6 GHz.

【0020】更に、光減衰器3の減衰量を1dBとし、
偏光軸の強度比を等しくするように半導体レーザの駆動
電流によって調整した場合の出射光間での干渉によるビ
ートノイズ周波数は4.5GHzとなる。
Further, the attenuation of the optical attenuator 3 is set to 1 dB,
When adjusted by the drive current of the semiconductor laser to make the intensity ratio of the polarization axes equal, the beat noise frequency due to the interference between the emitted lights is 4.5 GHz.

【0021】既に述べたように、本発明による偏光光源
装置は、どちらか一方の励起用半導体レーザの駆動電流
値(10GHz/A)を変えることにより、発振波長、
即ちビートノイズ周波数を容易に制御することが可能と
なる。
As described above, the polarized light source device according to the present invention changes the driving wavelength (10 GHz / A) of one of the pumping semiconductor lasers to change the oscillation wavelength,
That is, the beat noise frequency can be easily controlled.

【0022】[0022]

【発明の効果】以上説明したように、本発明によれば、
波長がわずかに異なり、偏波面が互いに垂直をなす二直
線偏光の光源装置において、ビートノイズ周波数を容易
に制御することが可能となり、レーザ媒質、厚みばらつ
きを相殺できる二直線偏光の光源装置を容易に作製する
ことが可能となる。その結果、出射光間での干渉による
ビートノイズ周波数の制御可能な二直線偏光光源を提供
することができる。
As described above, according to the present invention,
In a linearly polarized light source device whose wavelengths are slightly different and whose polarization planes are perpendicular to each other, it is possible to easily control the beat noise frequency, and to easily realize a linearly polarized light source device that can offset the laser medium and thickness variations. Can be manufactured. As a result, it is possible to provide a bilinearly polarized light source capable of controlling the beat noise frequency due to interference between the emitted lights.

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

【図1】本発明の実施の一形態に係る偏光光源装置の基
本構成を示す図。
FIG. 1 is a diagram showing a basic configuration of a polarized light source device according to one embodiment of the present invention.

【図2】従来の偏光光源装置の構成を示す図。FIG. 2 is a diagram showing a configuration of a conventional polarized light source device.

【図3】直線偏光光源の概略構成を示す図。FIG. 3 is a diagram showing a schematic configuration of a linearly polarized light source.

【符号の説明】[Explanation of symbols]

1,2,21,22 直線偏光光源 3 光減衰器 4,5,24,25 偏波保持ファイバ 6,26 光結合器 7,27 シングルモード光ファイバ 8 励起用半導体レーザ 9,13 光学レンズ 10,12 共振器ミラー 11 レーザ媒質 14 光共振器 1,2,21,22 Linearly polarized light source 3 Optical attenuator 4,5,24,25 Polarization maintaining fiber 6,26 Optical coupler 7,27 Single mode optical fiber 8 Pumping semiconductor laser 9,13 Optical lens 10, 12 cavity mirror 11 laser medium 14 optical cavity

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】 直線偏光を出射する二つの光源と、これ
らの光源から出射する二つ直線偏光を偏波面が互いに垂
直になるように合成する光結合器とを備えた偏光光源装
置において、前記二つの光源のうち少なくとも一方は光
の減衰機構を備えることを特徴とする偏光光源装置。
1. A polarized light source device comprising: two light sources that emit linearly polarized light; and an optical coupler that combines two linearly polarized light beams emitted from these light sources such that their polarization planes are perpendicular to each other. A polarized light source device, wherein at least one of the two light sources has a light attenuation mechanism.
【請求項2】 前記、二つの光源は半導体レーザ励起固
体レーザであることを特徴とする請求項1記載の偏光光
源装置。
2. The polarized light source device according to claim 1, wherein said two light sources are semiconductor laser pumped solid-state lasers.
【請求項3】 前記二つの光源における励起用半導体レ
ーザの駆動電流の値を異なるように設定した場合に、前
記光結合器から出射する、偏波面が互いに垂直な二つの
直線偏光の強度が等しくなるように、前記減衰機構の減
衰量が設定できることを特徴とする請求項2記載の偏光
光源装置。
3. When the values of the drive currents of the pumping semiconductor lasers in the two light sources are set differently, the intensities of the two linearly polarized light beams emitted from the optical coupler and whose polarization planes are perpendicular to each other are equal. 3. The polarized light source device according to claim 2, wherein the amount of attenuation of the attenuation mechanism can be set such that the amount of attenuation is adjusted.
JP2000193677A 2000-06-28 2000-06-28 Polarized light source device Pending JP2002016308A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2000193677A JP2002016308A (en) 2000-06-28 2000-06-28 Polarized light source device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2000193677A JP2002016308A (en) 2000-06-28 2000-06-28 Polarized light source device

Publications (1)

Publication Number Publication Date
JP2002016308A true JP2002016308A (en) 2002-01-18

Family

ID=18692628

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2000193677A Pending JP2002016308A (en) 2000-06-28 2000-06-28 Polarized light source device

Country Status (1)

Country Link
JP (1) JP2002016308A (en)

Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0645682A (en) * 1992-07-23 1994-02-18 Fujitsu Ltd Optical amplifier
JPH0799477A (en) * 1993-06-28 1995-04-11 Fujitsu Ltd Optical transmission method for optical communication system, optical transmitter and method and device for optical amplification
JPH10117172A (en) * 1996-10-11 1998-05-06 Matsushita Electric Ind Co Ltd Optical transmission system
JPH10256627A (en) * 1997-03-13 1998-09-25 Tokin Corp Semiconductor laser pumped solid laser light source
JPH11312848A (en) * 1998-02-27 1999-11-09 Fujitsu Ltd Optical amplifier

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0645682A (en) * 1992-07-23 1994-02-18 Fujitsu Ltd Optical amplifier
JPH0799477A (en) * 1993-06-28 1995-04-11 Fujitsu Ltd Optical transmission method for optical communication system, optical transmitter and method and device for optical amplification
JPH10117172A (en) * 1996-10-11 1998-05-06 Matsushita Electric Ind Co Ltd Optical transmission system
JPH10256627A (en) * 1997-03-13 1998-09-25 Tokin Corp Semiconductor laser pumped solid laser light source
JPH11312848A (en) * 1998-02-27 1999-11-09 Fujitsu Ltd Optical amplifier

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