JPH0563657A - Double balanced polarized wave diversity receiver - Google Patents

Double balanced polarized wave diversity receiver

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Publication number
JPH0563657A
JPH0563657A JP4031751A JP3175192A JPH0563657A JP H0563657 A JPH0563657 A JP H0563657A JP 4031751 A JP4031751 A JP 4031751A JP 3175192 A JP3175192 A JP 3175192A JP H0563657 A JPH0563657 A JP H0563657A
Authority
JP
Japan
Prior art keywords
light
optical
polarization
light receiving
local oscillation
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.)
Granted
Application number
JP4031751A
Other languages
Japanese (ja)
Other versions
JPH0828683B2 (en
Inventor
Hideo Kuwabara
秀夫 桑原
Terumi Chikama
輝美 近間
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.)
Fujitsu Ltd
Original Assignee
Fujitsu 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 Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP4031751A priority Critical patent/JPH0828683B2/en
Publication of JPH0563657A publication Critical patent/JPH0563657A/en
Publication of JPH0828683B2 publication Critical patent/JPH0828683B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Optical Communication System (AREA)
  • Radio Transmission System (AREA)

Abstract

PURPOSE:To attain reception of a stable coherent light by combining advantages of the polarized wave diversity reception system and the double balanced mixing system with respect to the double balanced polarized wave diversity receiver in the coherent light communication. CONSTITUTION:The receiver is provided with a polarized light separate means 3 separating a reception light 1 and a local oscillation light 2 into polarized components orthogonal to each other, photocouplers 5, 6 receiving the same polarized component in the optical signals separated respectively by the polarized light separate means 3, a light receiving means 4 converting the output optical signal mixed by the photocouplers 5, 6 into an electric signal, and a synthesis means 7 synthesizing the electric signal by the light receiving means 4 with phase adjustment or the like.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、コヒーレント光通信方
式に於ける二重平衡偏波ダイバーシティ受信装置に関す
る。光通信方式に於いては、光伝送路により伝送された
受信光を、直接的に受光素子により受光して電気信号に
変換する直接検波方式が一般的である。又コヒーレント
光通信方式に於いては、純度の高いレーザ光源を局部発
振光の光源とし、受信光と局部発振光とを混合するホモ
ダイン検波方式又はヘテロダイン検波方式が知られてお
り、直接検波方式に比較して受信感度の向上が期待でき
る。従って、光伝送路に於ける中継間隔の増大又は中継
器数の削減が可能となる。又加入者系等に適用した場合
に、分岐数の増大が期待できるから、光伝送路を経済的
に構成することが可能となる。このようなホモダイン検
波方式又はヘテロダイン検波方式を用いた時に、光伝送
路に於ける偏波揺らぎに起因する受信光と局部発振光と
の干渉効率の低下及び局部発振光の強度雑音による受信
感度の低下を抑制することが要望されている。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a dual balanced polarization diversity receiver in a coherent optical communication system. In the optical communication system, a direct detection system is generally used in which received light transmitted through an optical transmission line is directly received by a light receiving element and converted into an electric signal. Further, in the coherent optical communication system, a homodyne detection method or a heterodyne detection method in which a laser light source with high purity is used as a light source of local oscillation light and the received light and the local oscillation light are mixed is known, and the direct detection method is known. It can be expected that the receiving sensitivity will be improved in comparison. Therefore, it is possible to increase the repeater interval or reduce the number of repeaters in the optical transmission line. Further, when applied to a subscriber system or the like, an increase in the number of branches can be expected, so that the optical transmission line can be economically constructed. When using such a homodyne detection method or a heterodyne detection method, the reception efficiency due to the intensity noise of the local oscillation light and the reduction of the interference efficiency between the reception light and the local oscillation light due to the polarization fluctuation in the optical transmission line It is desired to suppress the decrease.

【0002】[0002]

【従来の技術】図3はコヒーレント光通信の説明図であ
り、ホモダイン検波方式又はヘテロダイン検波方式を示
すもので、送信部31からの光信号は、シングルモード
光ファイバからなる光伝送路32により受信部に伝送さ
れる。受信部に於いては、その受信光と、局部発振レー
ザ34からの局部発振光とを光混合器33に加えて混合
させ、その混合出力光をホトダイオード等の受光素子3
5に入射させ、光信号を電気信号に変換して増幅器36
に加えるものである。この増幅器36の出力信号は、例
えば、数GHzの中間周波信号となる。
2. Description of the Related Art FIG. 3 is an explanatory diagram of coherent optical communication, showing a homodyne detection system or a heterodyne detection system, in which an optical signal from a transmission unit 31 is received by an optical transmission line 32 formed of a single mode optical fiber. Transmitted to the department. In the receiving section, the received light and the local oscillation light from the local oscillation laser 34 are added to the optical mixer 33 and mixed, and the mixed output light is received by the light receiving element 3 such as a photodiode.
5 to convert the optical signal into an electric signal, and the amplifier 36
In addition to. The output signal of the amplifier 36 is, for example, an intermediate frequency signal of several GHz.

【0003】このようなコヒーレント光通信方式に於い
て、送信部31から送出された光信号は、レーザ光を直
接或いは間接に変調したもので、直線偏波光となるもの
であるが、通常のシングルモード光ファイバからなる長
距離の光伝送路32を伝搬することにより、楕円偏波光
となったり、或いは偏波方向が回転したりすることがあ
る。この偏波方向の揺らぎが大きいと、光混合器33に
於ける局部発振光との干渉効率が低下して、最悪状態で
は受信不可能となる。
In such a coherent optical communication system, the optical signal sent from the transmitter 31 is a laser beam that is directly or indirectly modulated and becomes a linearly polarized light. Propagation through the long-distance optical transmission line 32 formed of a mode optical fiber may result in elliptical polarized light, or the polarization direction may rotate. If this fluctuation in the polarization direction is large, the efficiency of interference with the locally oscillated light in the optical mixer 33 decreases, and reception becomes impossible in the worst state.

【0004】図4に示す偏波ダイバーシティ受信方式
は、このような問題点を解決しようとするものであり、
光伝送路を介して受信した受信光を、偏光分離素子41
によって直交する偏波成分に分離し、それぞれの偏波成
分に対して局部発振レーザ44からの局部発振光を光混
合器43,46により混合する。この場合、同一の局部
発振光から直交した偏波成分を形成する為に、光混合器
43,46間に1/2波長板45等の手段を設けるもの
であり、又偏光分離素子41と、光混合器46との配置
位置が図示のようになる場合、反射板42を設けて、偏
光分離素子41により分離された光信号を光混合器46
に入射させるものである。
The polarization diversity receiving system shown in FIG. 4 is intended to solve such a problem.
The received light received via the optical transmission line is converted into the polarization separation element 41.
The polarized light components are separated into orthogonal polarization components by, and the local oscillation light from the local oscillation laser 44 is mixed with the respective polarization components by the optical mixers 43 and 46. In this case, in order to form orthogonal polarization components from the same local oscillation light, means such as a ½ wavelength plate 45 is provided between the optical mixers 43 and 46, and the polarization separation element 41 and When the arrangement position with the light mixer 46 is as shown in the figure, the reflection plate 42 is provided and the optical signal separated by the polarization separation element 41 is supplied to the light mixer 46.
Is to be incident on.

【0005】光混合器43,46のそれぞれの出力光
は、受光素子47,48に入射されて電気信号に変換さ
れ、増幅器49,50により増幅される。合成部52に
於いては、増幅器49の出力信号と、移相器51により
位相が制御された増幅器50の出力信号とを合成するも
のであり、その合成出力信号が最大となるように、移相
器51の移相量が制御される。従って、光伝送路に於け
る偏波方向の揺らぎが大きい場合でも、受光素子47,
48の何れか一方から出力信号が得られるので、受信不
能となることはない。
The respective output lights of the light mixers 43 and 46 are incident on the light receiving elements 47 and 48, converted into electric signals, and amplified by the amplifiers 49 and 50. The synthesizing section 52 synthesizes the output signal of the amplifier 49 and the output signal of the amplifier 50 whose phase is controlled by the phase shifter 51, and shifts so that the synthesized output signal becomes maximum. The amount of phase shift of the phase shifter 51 is controlled. Therefore, even when the fluctuation of the polarization direction in the optical transmission line is large, the light receiving element 47,
Since the output signal can be obtained from any one of the 48, the reception is not impossible.

【0006】又図5は局部発振光の強度雑音によるC/
N特性曲線図を示し、図3又は図4に示す従来例に於い
て、局部発振レーザ34,44の局部発振光強度を大き
くするに従ってC/N又は最小受信レベルが改善される
ことを示す。しかし、局部発振レーザ34,44の安定
性等に基づく局部発振光の強度雑音が大きい場合、局部
発振光強度を大きくしても、本来到達できるショット雑
音限界に達しないのでC/Nが劣化することがある。従
って、強度雑音の小さい局部発振光を用いてC/Nの劣
化を許容するか、或いはこの強度雑音を抑圧する必要が
ある。
FIG. 5 shows C / due to the intensity noise of the local oscillation light.
An N characteristic curve diagram is shown, showing that the C / N or the minimum reception level is improved as the local oscillation light intensity of the local oscillation lasers 34, 44 is increased in the conventional example shown in FIG. 3 or 4. However, when the intensity noise of the locally oscillated light based on the stability of the locally oscillated lasers 34 and 44 is large, the shot noise limit that can be originally reached is not reached even if the intensity of the locally oscillated light is increased, so that the C / N is deteriorated. Sometimes. Therefore, it is necessary to allow the deterioration of C / N by using the local oscillation light having a small intensity noise or to suppress the intensity noise.

【0007】そこで、二重平衡混合方式が提案された。
この二重平衡混合方式は、例えば、図6に示すように、
受信光61と局部発振レーザ64からの局部発振光とを
光混合器62に加えて混合した時に、二つの出力光が得
られるから、それぞれ受光素子63,65にそれらの出
力光を入射して電気信号に変換し、増幅器66,67に
より増幅して減算器68に加えるものである。
Therefore, a double balanced mixing system has been proposed.
This double equilibrium mixing method is, for example, as shown in FIG.
When the reception light 61 and the local oscillation light from the local oscillation laser 64 are added to and mixed with the optical mixer 62, two output lights are obtained. Therefore, the output lights are incident on the light receiving elements 63 and 65, respectively. It is converted into an electric signal, amplified by the amplifiers 66 and 67, and added to the subtractor 68.

【0008】光混合器62から受光素子63,65に入
射される受信光と局部発振光とのビート信号成分は、1
80°位相がずれており、又局部発振光の強度雑音成分
は同相となるから、減算器68により増幅器66,67
の出力信号の差を求めることにより、ビート信号成分は
相加され、反対に強度雑音成分は相殺されて、局部発振
光の強度雑音を大幅に低減することができる。
The beat signal component of the received light and the local oscillation light which are incident on the light receiving elements 63 and 65 from the light mixer 62 is 1
Since the phase is shifted by 80 ° and the intensity noise components of the local oscillation light are in phase, the subtracter 68 causes the amplifiers 66 and 67 to operate.
By calculating the difference between the output signals of, the beat signal components are added and the intensity noise components are canceled, and the intensity noise of the local oscillation light can be greatly reduced.

【0009】図7は二重平衡受光部の説明図であり、
(A)は、光混合器71に受信光と局部発振光とが入射
され、混合光は直列接続の受光素子72,73に入射さ
れ、受光素子72,73の接続点から信号を増幅器74
に入力するものであり、受光素子72,73を直列に接
続したことにより、図6に於ける減算器68と同様に、
180°位相差のビート信号成分を相加し、反対に、同
相の強度雑音成分を相殺するように動作することにな
る。
FIG. 7 is an explanatory view of the double balanced light receiving section,
In (A), the received light and the local oscillation light are incident on the optical mixer 71, the mixed light is incident on the light receiving elements 72 and 73 connected in series, and a signal is amplified from the connection point of the light receiving elements 72 and 73 by the amplifier 74.
The light receiving elements 72 and 73 are connected in series, so that, like the subtracter 68 in FIG.
The beat signal components having a 180 ° phase difference are added, and on the contrary, the in-phase intensity noise components are canceled.

【0010】又図7の(B)は、3dB光カプラ75を
光混合器として用いた二重平衡受光部の場合を示し、受
信光と局部発振光とを3dB光カプラ75に入射し、混
合された出力光をそれぞれ直列接続の受光素子76,7
7に入射し、受光素子76,77の接続点の信号を増幅
器78により増幅するものであり、(A)に示す構成と
同様に、強度雑音を低減することができる。
Further, FIG. 7B shows a case of a double balanced light receiving section using the 3 dB optical coupler 75 as an optical mixer, in which the received light and the local oscillation light are incident on the 3 dB optical coupler 75 and mixed. The output light thus generated is connected in series to the light receiving elements 76, 7 respectively.
The signal incident on the light receiving element 7 and amplified at the connection point between the light receiving elements 76 and 77 is amplified by the amplifier 78, and the intensity noise can be reduced as in the configuration shown in FIG.

【0011】[0011]

【発明が解決しようとする問題点】前述の図3及び図4
に示す従来例に於いては、光混合器33,46からの一
方の混合出力光のみを利用し、他方の混合出力光は損失
となる。又局部発振光の強度雑音によるC/Nの劣化が
生じる。従って、受信感度を向上させることが困難であ
った。又図6に示す従来例に於いては、局部発振光の強
度雑音を抑圧することができるが、偏波方向の揺らぎに
よる受信感度の変動が生じて、最悪の場合は、受信光と
局部発振光との偏波方向が直交する状態となり、受信不
能となる場合が生じる欠点があった。本発明は、偏波ダ
イバーシティ受信方式と二重平衡混合方式との利点を組
合せて、安定なコヒーレント光受信を可能とすることを
目的とする。
Problems to be Solved by the Invention FIG. 3 and FIG.
In the conventional example shown in (1), only one mixed output light from the optical mixers 33 and 46 is used, and the other mixed output light is lost. In addition, the C / N is deteriorated due to the intensity noise of the local oscillation light. Therefore, it is difficult to improve the reception sensitivity. Further, in the conventional example shown in FIG. 6, the intensity noise of the local oscillation light can be suppressed, but the fluctuation of the reception sensitivity due to the fluctuation of the polarization direction occurs, and in the worst case, the reception light and the local oscillation are generated. There is a drawback that the polarization direction of light becomes orthogonal to each other, and the reception becomes impossible. It is an object of the present invention to combine the advantages of the polarization diversity reception system and the double balanced mixing system to enable stable coherent optical reception.

【0012】[0012]

【課題を解決するための手段】本発明の二重平衡偏波ダ
イバーシティ受信装置は、図1を参照して説明すると、
受信光1と局部発振光2とを互いに直交する偏光成分に
分離する複屈折結晶からなる偏光分離手段3と、この偏
光分離手段3から出力される各偏光成分のうち、一致し
た偏光成分同志を混合して複数の光信号を出力する光カ
プラ5,6と、これらの光カプラ5,6からの出力光信
号を中間周波数成分を有する電気信号に変換する受光手
段4と、この受光手段からの電気信号を位相調整して合
成する合成手段7とを備えたものである。
A dual balanced polarization diversity receiver according to the present invention will be described with reference to FIG.
Of the polarization components output from the polarization splitting means 3 and the polarization splitting means 3 formed of a birefringent crystal for splitting the received light 1 and the local oscillation light 2 into polarization components orthogonal to each other, the same polarization component Optical couplers 5 and 6 that mix and output a plurality of optical signals, light receiving means 4 that converts the output optical signals from these optical couplers 5 and 6 into an electrical signal having an intermediate frequency component, and the light receiving means from this light receiving means. And a synthesizing means 7 for synthesizing the electrical signals by adjusting their phases.

【0013】[0013]

【作用】偏光分離手段3は、複屈折結晶の板やブロック
等により構成され、受信光1と局部発振光2とを入射す
ると、それぞれ直交する偏光成分に分離する。その中の
同一偏光成分の受信光と局部発振光とを光カプラ5,6
に入射して混合する。その混合出力光信号を受光手段4
に入射することにより、中間周波数成分を有する電気信
号に変換されて合成手段7に入力される。この合成手段
7又は受光手段4の接続構成により、局部発振光の強度
雑音成分が相殺され、ビート信号成分が相加されるよう
に、同一偏光成分対応の電気信号が合成される。更に、
合成手段7に於いて、同一偏光成分対応の電気信号の合
成出力信号が、位相調整されて合成されて出力される。
それによって、偏波方向の揺らぎによる影響が除かれ
る。
The polarized light separating means 3 is composed of a birefringent crystal plate or block, and when the received light 1 and the locally oscillated light 2 are incident, they are separated into orthogonal polarized light components. The received light of the same polarization component and the locally oscillated light among them are converted into optical couplers 5, 6
Incident on and mixed. The mixed output optical signal is received by the light receiving means 4
When it is incident on, it is converted into an electric signal having an intermediate frequency component and input to the synthesizing means 7. Due to the connection configuration of the synthesizing means 7 or the light receiving means 4, the electric signals corresponding to the same polarization component are synthesized so that the intensity noise component of the local oscillation light is canceled and the beat signal component is added. Furthermore,
In the synthesizing means 7, the synthesized output signals of the electric signals corresponding to the same polarization component are phase-adjusted and synthesized and output.
This eliminates the effect of fluctuations in the polarization direction.

【0014】[0014]

【実施例】図2は本発明の実施例の説明図であり、11
は送信部、12は光伝送路、13は偏光分離手段を構成
する偏光ビームスプリッタ、14は局部発振レーザ、1
5,16は3dB光カプラ等の光カプラ、17〜20は
受光手段を構成する受光素子、21は合成手段を構成す
る合成回路である。
EXAMPLE FIG. 2 is an explanatory view of an example of the present invention.
Is a transmission unit, 12 is an optical transmission line, 13 is a polarization beam splitter which constitutes polarization separation means, 14 is a local oscillation laser, 1
Reference numerals 5 and 16 are optical couplers such as 3 dB optical couplers, 17 to 20 are light receiving elements that constitute light receiving means, and 21 is a combining circuit that constitutes combining means.

【0015】送信部11からの光信号が光伝送路12を
介して受信部の偏光ビームスプリッタ13に入射され、
直交する偏光成分、即ち、P波とS波とに分離される。
又局部発振レーザ14からの局部発振光も偏光ビームス
プリッタ13に入射されて、直交する偏光成分、即ち、
P波とS波とに分離される。この偏光ビームスプリッタ
13は、複屈折結晶により構成され、1枚の板状の場合
を図示しているが、光カプラ16との関係配置に対応し
てブロック状等の各種の形状を採用することができる。
The optical signal from the transmitter 11 is incident on the polarization beam splitter 13 of the receiver via the optical transmission line 12,
It is separated into orthogonal polarization components, that is, P wave and S wave.
Further, the locally oscillated light from the locally oscillated laser 14 is also incident on the polarization beam splitter 13, and orthogonal polarization components, that is,
It is separated into P wave and S wave. The polarization beam splitter 13 is made of a birefringent crystal and is illustrated as a single plate, but various shapes such as a block may be adopted according to the relational arrangement with the optical coupler 16. You can

【0016】偏光ビームスプリッタ13により分離され
た直交する偏光成分のうちの同一の偏光成分の受信光と
局部発振光とを、光カプラ15,16にそれぞれ入射す
る。例えば、受信光のS波と局部発振光のS波とを光カ
プラ15に入射して混合し、受信光のP波と局部発振光
のP波とを光カプラ16に入射して混合する。これらの
光カプラ15,16は、光導波路型等の構成を用いるこ
とができる。
The received light and the local oscillation light having the same polarization component of the orthogonal polarization components separated by the polarization beam splitter 13 are made incident on the optical couplers 15 and 16, respectively. For example, the S wave of the received light and the S wave of the locally oscillated light are incident on the optical coupler 15 and mixed, and the P wave of the received light and the P wave of the locally oscillated light are incident on the optical coupler 16 and mixed. These optical couplers 15 and 16 can use an optical waveguide type structure or the like.

【0017】光カプラ15により混合されたS波は受光
素子17,18に入射され、光カプラ16により混合さ
れたP波は受光素子19,20に入射されて、それぞれ
電気信号に変換される。受光素子17,18は直列に接
続され、その接続点は合成回路21に接続され、又受光
素子19,29は直列に接続され、その接続点は合成回
路21に接続されている。この場合、受光素子17,1
8に入射される局部発振光の強度雑音は同相となり、又
受光素子19,20に入射される局部発振光の強度雑音
も同相となる。又ビート信号成分はそれぞれ180°の
位相差となる。従って、直列に接続された受光素子1
7,18及び19,20により、局部発振光の強度雑音
は相殺され、ビート信号成分は相加されることになる。
The S wave mixed by the optical coupler 15 is incident on the light receiving elements 17 and 18, and the P wave mixed by the optical coupler 16 is incident on the light receiving elements 19 and 20 and converted into electric signals. The light receiving elements 17 and 18 are connected in series, the connection point is connected to the combining circuit 21, and the light receiving elements 19 and 29 are connected in series, and the connection point is connected to the combining circuit 21. In this case, the light receiving elements 17, 1
The intensity noise of the locally oscillated light entering 8 is in phase, and the intensity noise of the locally oscillated light incident on the light receiving elements 19 and 20 is also in phase. The beat signal components have a phase difference of 180 °. Therefore, the light receiving elements 1 connected in series
7, 18 and 19, 20 cancel the intensity noise of the local oscillation light and add the beat signal components.

【0018】合成回路21は、受光素子17,18及び
19,20の出力信号の位相を調整して合成するもので
あり、その場合に、図4に示すように、合成出力信号が
最大となるように、移相器を制御することになる。それ
によって、P波とS波との成分が合成されるから、光伝
送路12による偏波方向の揺らぎが生じたとしても、安
定な受信が可能となる。
The combining circuit 21 adjusts the phases of the output signals of the light receiving elements 17, 18 and 19, 20 and combines the output signals. In this case, the combined output signal becomes maximum as shown in FIG. Thus, it will control the phase shifter. As a result, the components of the P wave and the S wave are combined, so that stable reception is possible even if fluctuations in the polarization direction due to the optical transmission line 12 occur.

【0019】[0019]

【発明の効果】以上説明したように、本発明は、複屈折
結晶からなる偏光分離手段3により、受信光1と局部発
振光2とをそれぞれ直交する偏光成分に分離し、それぞ
れの偏光成分のうちの同一の偏光成分同志を光カプラ
5,6により混合し、それぞれの光カプラ5,6から出
力される光信号をホトダイオード等からなる受光手段4
により中間周波数成分を有する電気信号に変換し、合成
手段7により位相調整等を行って合成するものであり、
局部発振光の強度雑音は、同相で入力される受光手段4
の受光素子の出力信号の差を求めることにより相殺され
る。その時、ビート信号成分は180°位相であるから
相加されることになる。従って、雑音強度の大きい半導
体レーザ等を局部発振レーザとして用いることが可能と
なり、コストダウンを図ることができる。
As described above, according to the present invention, the polarized light separating means 3 made of a birefringent crystal separates the received light 1 and the locally oscillated light 2 into polarized light components which are orthogonal to each other. The same polarization components among them are mixed by the optical couplers 5 and 6, and the optical signals output from the optical couplers 5 and 6 are received by the light receiving means 4 including a photodiode or the like.
Is converted into an electric signal having an intermediate frequency component, and the synthesizing means 7 performs phase adjustment and the like to synthesize.
The intensity noise of the local oscillation light is input in phase with the light receiving means 4
This is canceled by obtaining the difference between the output signals of the light receiving elements. At that time, since the beat signal components are 180 ° in phase, they are added. Therefore, a semiconductor laser or the like having high noise intensity can be used as the local oscillation laser, and the cost can be reduced.

【0020】又伝送路等による偏波方向の揺らぎの影響
は、合成手段7に於けるP波とS波との成分の電気信号
の位相調整による合成によって除くことができる。従っ
て、安定なコヒーレント光通信を行うことができる利点
がある。又偏光分離手段3を図示のように板状に形成
し、光カプラ5,6を導波路型とすることにより、それ
らの間を直接光学的に結合することも容易となり、又光
カプラ5,6と受光手段4の各受光素子とを直接に光結
合させることも可能であり、全体の小型化を図ることが
できる利点がある。
The influence of fluctuations in the polarization direction due to the transmission line or the like can be eliminated by combining the electric signals of the P wave and S wave components in the combining means 7 by adjusting the phase. Therefore, there is an advantage that stable coherent optical communication can be performed. Further, by forming the polarization separating means 3 in a plate shape as shown in the drawing and making the optical couplers 5 and 6 of the waveguide type, it becomes easy to directly optically couple them, and the optical couplers 5 and 6 can be easily coupled. It is also possible to directly optically couple 6 and each light receiving element of the light receiving means 4, and there is an advantage that the overall size can be reduced.

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

【図1】本発明の原理説明図である。FIG. 1 is a diagram illustrating the principle of the present invention.

【図2】本発明の実施例の説明図である。FIG. 2 is an explanatory diagram of an example of the present invention.

【図3】コヒーレント光通信の説明図である。FIG. 3 is an explanatory diagram of coherent optical communication.

【図4】偏波ダイバーシティ受信方式の説明図である。FIG. 4 is an explanatory diagram of a polarization diversity receiving system.

【図5】局部発振光の強度雑音によるC/N特性曲線図
である。
FIG. 5 is a C / N characteristic curve diagram due to intensity noise of local oscillation light.

【図6】二重平衡混合方式の説明図である。FIG. 6 is an explanatory diagram of a double equilibrium mixing system.

【図7】二重平衡受光部の説明図である。FIG. 7 is an explanatory diagram of a double balanced light receiving unit.

【符号の説明】[Explanation of symbols]

1 受信光 2 局部発振光 3 偏光分離手段 4 受光手段 5,6 光カプラ 7 合成手段 1 Received Light 2 Local Oscillation Light 3 Polarization Separation Means 4 Light Receiving Means 5, 6 Optical Coupler 7 Combining Means

───────────────────────────────────────────────────── フロントページの続き (51)Int.Cl.5 識別記号 庁内整理番号 FI 技術表示箇所 H04B 10/18 ─────────────────────────────────────────────────── ─── Continuation of the front page (51) Int.Cl. 5 Identification code Office reference number FI technical display location H04B 10/18

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 受信光(1)及び局部発振光(2)を互
いに直交する偏光成分に分離する複屈折結晶からなる偏
光分離手段(3)と、 該偏光分離手段から出力される各偏光成分のうち、一致
した偏光成分同志を混合して複数の光信号を出力する光
カプラ(5,6)と、 該光カプラ(5,6)からの出力光信号を中間周波数成
分を有する電気信号に変換する受光手段(4)と、 該受光手段(4)からの電気信号を位相調整して合成す
る合成手段(7)とを備えたことを特徴とする二重平衡
偏波ダイバーシティ受信装置。
1. A polarization separation means (3) made of a birefringent crystal for separating the received light (1) and the local oscillation light (2) into polarization components orthogonal to each other, and each polarization component output from the polarization separation means. Among them, an optical coupler (5, 6) that mixes the same polarization components and outputs a plurality of optical signals, and an output optical signal from the optical coupler (5, 6) into an electric signal having an intermediate frequency component. A dual balanced polarization diversity receiver comprising a light receiving means (4) for converting and a combining means (7) for phase-adjusting and combining the electric signals from the light receiving means (4).
JP4031751A 1992-02-19 1992-02-19 Double balanced polarization diversity receiver Expired - Lifetime JPH0828683B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4031751A JPH0828683B2 (en) 1992-02-19 1992-02-19 Double balanced polarization diversity receiver

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4031751A JPH0828683B2 (en) 1992-02-19 1992-02-19 Double balanced polarization diversity receiver

Related Parent Applications (1)

Application Number Title Priority Date Filing Date
JP61163717A Division JPH0671232B2 (en) 1986-06-20 1986-07-14 Double balanced polarization diversity receiver

Publications (2)

Publication Number Publication Date
JPH0563657A true JPH0563657A (en) 1993-03-12
JPH0828683B2 JPH0828683B2 (en) 1996-03-21

Family

ID=12339729

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4031751A Expired - Lifetime JPH0828683B2 (en) 1992-02-19 1992-02-19 Double balanced polarization diversity receiver

Country Status (1)

Country Link
JP (1) JPH0828683B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2009060526A1 (en) * 2007-11-08 2009-05-14 Fujitsu Limited Coherent optical receiver

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62200831A (en) * 1986-02-28 1987-09-04 Nippon Telegr & Teleph Corp <Ntt> Optical heterodyne/homodyne reception circuit

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62200831A (en) * 1986-02-28 1987-09-04 Nippon Telegr & Teleph Corp <Ntt> Optical heterodyne/homodyne reception circuit

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2009060526A1 (en) * 2007-11-08 2009-05-14 Fujitsu Limited Coherent optical receiver

Also Published As

Publication number Publication date
JPH0828683B2 (en) 1996-03-21

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