JPS63136839A - Tuning type optical receiver - Google Patents
Tuning type optical receiverInfo
- Publication number
- JPS63136839A JPS63136839A JP61285308A JP28530886A JPS63136839A JP S63136839 A JPS63136839 A JP S63136839A JP 61285308 A JP61285308 A JP 61285308A JP 28530886 A JP28530886 A JP 28530886A JP S63136839 A JPS63136839 A JP S63136839A
- Authority
- JP
- Japan
- Prior art keywords
- amplifier
- tuning
- frequency
- tuned
- circuit
- 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
- 230000003287 optical effect Effects 0.000 title claims description 20
- 230000001939 inductive effect Effects 0.000 claims abstract description 12
- 230000005540 biological transmission Effects 0.000 abstract description 9
- 230000003321 amplification Effects 0.000 abstract description 4
- 238000003199 nucleic acid amplification method Methods 0.000 abstract description 4
- 230000001427 coherent effect Effects 0.000 description 5
- 238000004891 communication Methods 0.000 description 5
- 238000010586 diagram Methods 0.000 description 5
- 238000001514 detection method Methods 0.000 description 4
- 238000001228 spectrum Methods 0.000 description 3
- 239000003990 capacitor Substances 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
Abstract
Description
【発明の詳細な説明】
〔概 要〕
コヒーレント光通信へテロダイン検波方式に用いられる
光受信器に、共振周波数の異なる複数の同調増幅回路を
多段接続したものを用い、所要帯域幅を得て高ビツトレ
ート伝送を可能とする。[Detailed Description of the Invention] [Summary] An optical receiver used in a coherent optical communication heterodyne detection method is equipped with a plurality of tuned amplifier circuits with different resonance frequencies connected in multiple stages to obtain the required bandwidth and achieve high Enables bit rate transmission.
本発明はコヒーレント光通信ヘテロダイン検波方式に用
いる同調型光受信器に関するもので、さらに詳しく言え
ば、共振周波数の異なる複数の同調増幅回路を多段接続
して所要帯域幅を得て高ビツトレート伝送を可能とした
同調型光受信器に関するものである。The present invention relates to a tunable optical receiver used in a coherent optical communication heterodyne detection method. More specifically, the present invention relates to a tunable optical receiver used in a coherent optical communication heterodyne detection method. More specifically, a plurality of tunable amplifier circuits with different resonance frequencies are connected in multiple stages to obtain the required bandwidth and enable high bit rate transmission. This invention relates to a tunable optical receiver.
高速に多量の情報を伝達するためにコヒーレント光によ
る通信方式が利用されている。特にコヒーレント光通信
ヘテロゲイン検波方式を用いるものにあっては、信号光
と局発光とを重ね合わせて中間周波数信号を形成してい
る。例えば、信号光及び局発光として使用するレーザの
波長を1オングストロームオーダー迄調整した場合、中
間周波数が凡そ10GHzとなる。従って中間周波数自
体が非常に高い周波数であるので、信号光を受光する光
受信器のフロントエンドとして極めて高い周波数範囲迄
、応答可能なものが要求される。フロントエンドとして
一般にベースバンド伝送に用いられている受信回路を用
いると、極めて広帯域のものが必要とされる。このよう
な広帯域受信回路を用いない場合は、中間周波数の周囲
に広がる信号スペクトルのみを通過可能な光受信器を構
成する必要がある。Communication systems using coherent light are used to transmit large amounts of information at high speed. Particularly in those using a coherent optical communication heterogain detection method, the signal light and the local light are superimposed to form an intermediate frequency signal. For example, if the wavelength of the laser used as the signal light and the local light is adjusted to the order of 1 angstrom, the intermediate frequency will be approximately 10 GHz. Therefore, since the intermediate frequency itself is a very high frequency, a front end of an optical receiver that receives signal light is required to be capable of responding to an extremely high frequency range. If a reception circuit generally used for baseband transmission is used as a front end, an extremely wide band is required. If such a wideband receiving circuit is not used, it is necessary to configure an optical receiver that can pass only the signal spectrum that spreads around the intermediate frequency.
光受信器のフロントエンドは、例えば第4図(alに示
すように受光素子IとFETl0と増@器2とより成る
ハイインピーダンス型、同図(blに示すように増幅器
2の出力からFETl0のゲートへ接続された帰還抵抗
5を備えるトランスインピーダンス型、あるいは同図(
C)に示すように受光素子1の容量成分と並列のコイル
6を備えて同調回路を構成したLC同開型等の形式のも
のが用いられている。ハイインピーダンス型及びトラン
スインピーダンス型のものは、第3図(blに示すよう
に、周波数特性がDC領域まで伸びた周波数特性を有す
る。一方、フロントエンドとしてLC同調型のものは、
第3図(C)に示すような周波数特性を有する。The front end of the optical receiver is, for example, a high-impedance type consisting of a photodetector I, FETl0, and amplifier 2 as shown in Figure 4 (al), or a high-impedance type consisting of a light receiving element I, FETl0, and amplifier 2 as shown in Fig. A transimpedance type with a feedback resistor 5 connected to the gate, or a transimpedance type (
As shown in C), an LC open circuit or the like is used, which includes a coil 6 in parallel with the capacitive component of the light receiving element 1 to form a tuned circuit. The high-impedance type and transimpedance type have frequency characteristics that extend to the DC region, as shown in Figure 3 (bl).On the other hand, the LC-tuned type as a front end has a frequency characteristic that extends to the DC region.
It has frequency characteristics as shown in FIG. 3(C).
この従来方式では、ハイインピーダンス型及びトランス
インピーダンス型のものにあっては、周波数特性がDC
領域まで伸びている故、中間周波数及び所要周波数帯域
の信号を歪みなく伝送することが可能になるが、そのた
めには、フロントエンドの周波数特性を極めて広帯域に
設計する必要があった。一方、フロントエンドとしてL
C同調型のものを用いる場合は、平坦部分が極めて少な
い周波数特性となる。従って高ビットレートで伝送を行
なうと、出力波形における符号量干渉が大きくなるので
、S/N比が低下するという問題があった。In this conventional method, the frequency characteristics of the high impedance type and transimpedance type are DC.
Since it extends over a wide range, it becomes possible to transmit signals in the intermediate frequency and required frequency bands without distortion, but in order to do so, it was necessary to design the frequency characteristics of the front end to have an extremely wide band. On the other hand, as a front end, L
When a C-tuned type is used, the frequency characteristic has extremely few flat parts. Therefore, when transmission is performed at a high bit rate, the amount of code interference in the output waveform becomes large, resulting in a problem that the S/N ratio decreases.
本発明はこのような点に鑑みて創作されたもので、高ビ
・ノドレート伝送に適した同開型光受信器を提供するこ
とを目的としている。The present invention was created in view of these points, and an object of the present invention is to provide a same-open type optical receiver suitable for high-node rate transmission.
第1図は本発明の同調型光受信器の原理ブロック回路図
を示す。FIG. 1 shows a basic block circuit diagram of a tunable optical receiver of the present invention.
図において1は容量成分を含む受光素子であり、2は増
幅器である。また、3は並列の誘導性素子及び容量性素
子から成る同調回路であり、4は誘導性素子である。受
光素子りの容量成分及び誘導性素子4から成る同調回路
に増幅器2が接続されて同調増幅器が形成され、該同調
増@器に同調回路3及び増幅器2から成る少なくとも1
つの同調増幅器が縦続接続されている。容量成分を含む
受光素子1と誘導性素子により形成される同調回路の共
振(同調)周波数と各同調回路3の共振周波数は各々少
しずつ異なるように調整されている。In the figure, 1 is a light receiving element including a capacitive component, and 2 is an amplifier. Further, 3 is a tuning circuit consisting of a parallel inductive element and a capacitive element, and 4 is an inductive element. An amplifier 2 is connected to a tuned circuit consisting of a capacitive component of the light receiving element and an inductive element 4 to form a tuned amplifier, and at least one of the tuned circuit 3 and the amplifier 2 is connected to the tuned amplifier 2.
Two tuned amplifiers are connected in cascade. The resonance (tuning) frequency of the tuning circuit formed by the light receiving element 1 including a capacitive component and the inductive element and the resonance frequency of each tuning circuit 3 are adjusted to be slightly different from each other.
なお、同図において受光素子1は容量成分を含むものと
して等測的に図示しである。Note that in the figure, the light receiving element 1 is illustrated isometrically as including a capacitive component.
容量成分を含む受光素子1と誘導性素子4により形成さ
れる同調回路の共振(同調)周波数の信号を増幅器2に
て増幅すると共に、縦続接続された同調回路3及び増幅
器2にてこれと少し異なる周波数の信号を同調増幅する
。さらに、縦続接続された同調回路3及び増幅器2にて
さらに少し異なる周波数の信号を同調増幅する。これに
て総合周波数特性は第3図(a)の実線に示すように、
所要の帯域幅を有するものとなる。The amplifier 2 amplifies the signal at the resonant (tuned) frequency of the tuned circuit formed by the photodetector 1 containing a capacitive component and the inductive element 4, and the cascaded tuned circuit 3 and amplifier 2 amplify the signal at the resonant (tuned) frequency. Tuned amplification of signals of different frequencies. Furthermore, the cascade-connected tuning circuit 3 and amplifier 2 further tune and amplify signals of slightly different frequencies. With this, the overall frequency characteristic is as shown by the solid line in Figure 3(a).
It will have the required bandwidth.
第2図は本発明の実施例であって、容量成分を含む受光
素子lと直列にバイアス抵抗7が接続されて示される。FIG. 2 shows an embodiment of the present invention, in which a bias resistor 7 is shown connected in series with a light receiving element l including a capacitive component.
バイアス抵抗7に並列にコイル4が並列接続されること
により、受光素子1の容量成分とコイル4の誘導成分と
により決まる共振周波数を有する第1の同調回路3が形
成される。この第1の同調回路3に増幅器2が接続され
て第1の同調増幅器が構成されている。増幅器2は2っ
のFET4.5より構成され、そのFET4によるソー
ス接地回路構成及びFET5によるソースフォロワ回路
構成によって高入力インピーダンス及び低出力インピー
ダンスの増幅器となっている。By connecting the coil 4 in parallel to the bias resistor 7, a first tuned circuit 3 having a resonant frequency determined by the capacitive component of the light receiving element 1 and the inductive component of the coil 4 is formed. An amplifier 2 is connected to this first tuning circuit 3 to constitute a first tuning amplifier. The amplifier 2 is composed of two FETs 4.5, and has a source grounding circuit configuration using the FET 4 and a source follower circuit configuration using the FET 5, making it an amplifier with high input impedance and low output impedance.
この第1の同調増幅器10に、同一構成の第2及び第3
の同調増幅器12.14が接続されている。This first tuned amplifier 10 has second and third tuned amplifiers having the same configuration.
Tuned amplifiers 12 and 14 are connected.
これら同調増幅器12.14はいずれも、LC同調回路
3と、第1の同調増幅器10の増幅器2と同一構成の増
幅器2とから構成されており、そのLC同調回路3の各
々の共振周波数は第1の同調増幅器10の同調回路3の
共振周波数を基準にしてそれに対し少しずつ異なるよう
に設定されている。このような設定により、本発明の同
調型光受信器の総合周波数特性は第3図(a)に示すよ
うになる。この周波数特性は高ビツトレート伝送に必要
な中間周波数近傍の信号スペクトル成分の伝送を可能に
するものである。この高ビツトレート伝送を可能にする
上述総合周波数特性は上述の如く、第1の同調増幅器1
0の共振周波数を基準とされるが、これは受光素子1の
容量成分がその素子固有の値をとることによる。従って
、他の同調増幅器の共振周波数はそれぞれ、第1の同調
増幅器10の共振周波数を基準として上述総合周波数特
性が得られるように決められる。つまり、それぞれのL
CC同量回路コンデンサの容量値及びコイルのインダク
タンス値が決められる。例えば、同調増幅器10の共振
周波数を中間周波数flFとした場合、コイル4のイン
ダクタンスは受光素子Iのキ、ヤパシタンスに対して決
められる。そして、同調増幅器I2の共振周波数は中間
周波数fTFの下側側に来るようにその同調回路3のL
及びCの値が決められ、同調増幅器I4の共振周波数は
中間周波数ftpの上側側に来るようにその同調回路3
のL及びCの値は決められる。These tuned amplifiers 12 and 14 each include an LC tuned circuit 3 and an amplifier 2 having the same configuration as the amplifier 2 of the first tuned amplifier 10, and the resonant frequency of each of the LC tuned circuits 3 is The resonant frequency of the tuned circuit 3 of the tuned amplifier 10 of No. 1 is set as a reference, and is set to be slightly different from the resonant frequency of the tuned circuit 3 of the tuned amplifier 10. With such settings, the overall frequency characteristic of the tunable optical receiver of the present invention becomes as shown in FIG. 3(a). This frequency characteristic makes it possible to transmit signal spectrum components near intermediate frequencies necessary for high bit rate transmission. The above-mentioned overall frequency characteristics that enable this high bit rate transmission are determined by the first tuning amplifier 1.
The resonance frequency of 0 is used as a reference, but this is because the capacitance component of the light receiving element 1 takes a value unique to that element. Therefore, the resonant frequencies of the other tuned amplifiers are determined based on the resonant frequency of the first tuned amplifier 10 so as to obtain the above-mentioned overall frequency characteristics. In other words, each L
The capacitance value of the CC equivalent circuit capacitor and the inductance value of the coil are determined. For example, when the resonant frequency of the tuned amplifier 10 is set to the intermediate frequency flF, the inductance of the coil 4 is determined with respect to the capacitance of the light receiving element I. Then, the L of the tuned circuit 3 is set so that the resonant frequency of the tuned amplifier I2 is below the intermediate frequency fTF.
and C are determined, and the tuning circuit 3 is set so that the resonant frequency of the tuned amplifier I4 is above the intermediate frequency ftp.
The values of L and C are determined.
この第2図に示す例では2段の同調増幅回路を用いてい
るが、さらに多段に構成することも可能である。また、
本発明は増幅素子に特定されるものでは無く、FETに
代えてこれに類するBJT等を□用いることができる。In the example shown in FIG. 2, a two-stage tuned amplifier circuit is used, but it is also possible to configure it with more stages. Also,
The present invention is not limited to an amplification element, and a similar BJT or the like can be used in place of the FET.
また、周波数特性が夫々異なる複数のLC同調回路を用
いて中間周波数段を構成すると、回路雑音の少ない光受
信器が得られる。Moreover, if an intermediate frequency stage is constructed using a plurality of LC tuning circuits each having different frequency characteristics, an optical receiver with less circuit noise can be obtained.
以上述べてきたように本発明によれば、光受信器を構成
する各段による総合周波数特性を中間周波数近傍の必要
な信号スペクトルを伝送可能なものとしたので、高ビツ
トレート伝送が可能となる。As described above, according to the present invention, the overall frequency characteristics of each stage constituting the optical receiver are made such that the necessary signal spectrum near the intermediate frequency can be transmitted, and therefore high bit rate transmission is possible.
第1図は本発明の同調型光受信器の原理ブロック回路図
、
第2図は本発明の実施例の回路図、
第3図は周波数特性図、
第4図(al〜(C1は従来例の回路図である。
第1図において、
1は受光素子、
2は増幅器、
3はLC同調回路、
4は誘導性素子(コイル)である。
第1図
/f罹β月の一実矛色イケJIIKB]周彼殺持・に図
第3図Fig. 1 is a principle block circuit diagram of the tunable optical receiver of the present invention, Fig. 2 is a circuit diagram of an embodiment of the present invention, Fig. 3 is a frequency characteristic diagram, Fig. 4 (al to (C1 is a conventional example) This is a circuit diagram. In Fig. 1, 1 is a light receiving element, 2 is an amplifier, 3 is an LC tuning circuit, and 4 is an inductive element (coil). [Ike JIIKB] Zhou He Murder and Figure 3
Claims (2)
(4)及び増幅器(2)より成る同調増幅回路と、 該同調増幅回路に縦続接続され前記同調増幅回路の共振
周波数と異なる周波数で共振する並列の誘導性素子及び
容量性素子(3)を含む少なくとも1つの同調増幅回路
とから成る同調型光受信器。(1) a light receiving element (1) containing a capacitive component; a tuned amplifier circuit consisting of an inductive element (4) and an amplifier (2) that together with the light receiving element (1) constitute a tuned circuit; and a tuned amplifier circuit connected in series to the tuned amplifier circuit; A tunable optical receiver comprising at least one tunable amplifier circuit connected in parallel and including an inductive element and a capacitive element (3) resonating at a frequency different from the resonant frequency of the tunable amplifier circuit.
イアス抵抗(7)を備え、該バイアス抵抗(7)にコイ
ル(4)が並列接続されて受光素子(1)の容量成分を
含む同調回路が構成されることを特徴とする特許請求の
範囲第1項記載の同調型光受信器。(2) A bias resistor (7) is provided for applying a bias current to the light receiving element (1), and a coil (4) is connected in parallel to the bias resistor (7) to tune the light receiving element (1) including its capacitive component. A tunable optical receiver according to claim 1, characterized in that a circuit is constructed.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP61285308A JPS63136839A (en) | 1986-11-28 | 1986-11-28 | Tuning type optical receiver |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP61285308A JPS63136839A (en) | 1986-11-28 | 1986-11-28 | Tuning type optical receiver |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS63136839A true JPS63136839A (en) | 1988-06-09 |
Family
ID=17689847
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP61285308A Pending JPS63136839A (en) | 1986-11-28 | 1986-11-28 | Tuning type optical receiver |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS63136839A (en) |
-
1986
- 1986-11-28 JP JP61285308A patent/JPS63136839A/en active Pending
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