JPS61148929A - Communication device - Google Patents
Communication deviceInfo
- Publication number
- JPS61148929A JPS61148929A JP59270707A JP27070784A JPS61148929A JP S61148929 A JPS61148929 A JP S61148929A JP 59270707 A JP59270707 A JP 59270707A JP 27070784 A JP27070784 A JP 27070784A JP S61148929 A JPS61148929 A JP S61148929A
- Authority
- JP
- Japan
- Prior art keywords
- light
- optical fiber
- line
- polarized wave
- 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
Links
- 238000004891 communication Methods 0.000 title claims abstract description 17
- 230000003287 optical effect Effects 0.000 claims abstract description 14
- 230000000694 effects Effects 0.000 claims abstract description 13
- 239000004020 conductor Substances 0.000 claims abstract description 10
- 230000001902 propagating effect Effects 0.000 claims description 5
- 238000001514 detection method Methods 0.000 claims 1
- 239000013307 optical fiber Substances 0.000 abstract description 20
- 230000005291 magnetic effect Effects 0.000 abstract description 5
- 230000010287 polarization Effects 0.000 abstract description 5
- 230000008878 coupling Effects 0.000 abstract description 3
- 238000010168 coupling process Methods 0.000 abstract description 3
- 238000005859 coupling reaction Methods 0.000 abstract description 3
- 230000000644 propagated effect Effects 0.000 abstract 1
- 230000005284 excitation Effects 0.000 description 4
- 238000010586 diagram Methods 0.000 description 3
- 230000001939 inductive effect Effects 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 239000013078 crystal Substances 0.000 description 1
- 230000005684 electric field Effects 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- 238000010295 mobile communication Methods 0.000 description 1
- 230000005298 paramagnetic effect Effects 0.000 description 1
- 239000000523 sample Substances 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04B—TRANSMISSION
- H04B10/00—Transmission systems employing electromagnetic waves other than radio-waves, e.g. infrared, visible or ultraviolet light, or employing corpuscular radiation, e.g. quantum communication
- H04B10/25—Arrangements specific to fibre transmission
Landscapes
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Engineering & Computer Science (AREA)
- Computer Networks & Wireless Communication (AREA)
- Signal Processing (AREA)
- Optical Communication System (AREA)
Abstract
Description
【発明の詳細な説明】
〈産業上の利用分野〉
本発明は光変調効果を有する光導体線路を用いた通信装
置に係名。DETAILED DESCRIPTION OF THE INVENTION <Industrial Application Field> The present invention relates to a communication device using a light guide line having a light modulation effect.
〈従来の技術〉
従来祉移動体に搭載した送受信装置のアンテナによって
、地上に布設された空間結合線路例えば、誘導無線線路
あるいは漏洩同軸ケーブルと電磁的に結合して、上記誘
導無線線路あるいは漏洩同軸ケーブルに接続された地上
局との間τ通信が行なわれる、いわゆる移動体通信は広
く行なわれて来た。<Prior art> Conventionally, an antenna of a transmitting/receiving device mounted on a mobile vehicle is electromagnetically coupled to a spatially coupled line laid on the ground, such as an inductive radio line or a leaky coaxial cable, and the above-mentioned inductive radio line or leaky coaxial cable is electromagnetically coupled. So-called mobile communication, in which τ communication is performed with a ground station connected to a cable, has been widely used.
〈発明が解決しようとする問題点〉
しバし地上の空間結合線路として光ファイバを用いたも
のはいまだ開発されていない。<Problems to be Solved by the Invention> However, nothing using optical fibers as a terrestrial spatial coupling line has yet been developed.
そこで本発明は上記の従来技術に鑑み、空間結合線路と
して光導体線路を用いた新しい通信装置を提供すること
を目的とする。本発明による通信装置はクレー”ン車輌
等の移動体と地上局間の通信、従来の誘導無線適用分野
にも広く適用できるものである。SUMMARY OF THE INVENTION In view of the above-mentioned prior art, it is an object of the present invention to provide a new communication device using a photoconductor line as a spatial coupling line. The communication device according to the present invention can be widely applied to communication between a mobile object such as a crane vehicle and a ground station, and to conventional guided radio application fields.
〈問題点を解決するための手段〉
本発明による通信装置は、光変調効果を有する光導体線
路、該光導体線路の入力端に設けられた光源、該光源の
光を直線偏光するヱ記光源と也導体線路入力端の間に設
けられ几偏光子、上記光導体線路の出力端に設けられた
検光子、該検光子の出力信号を電気信号に変換する受光
素子並びに、該受光素子に復調器を介して接続された受
信機からなる受信側装置と、送信機並びに、該送信器に
変調器を介して接続され上記光導体線路を伝搬する直線
偏光を光変調する光変調器からなる送信側装置とからな
り、該送信側装置から発信された信号によって、上記光
導体線路を伝搬する直線偏光を光変調し、光変調された
変調成分を、上記受信側装置によって検出・受信するこ
とを%徴とするものである。<Means for Solving the Problems> A communication device according to the present invention comprises a light guide line having a light modulation effect, a light source provided at the input end of the light guide line, and the light source described above that linearly polarizes light from the light source. A polarizer provided between the input end of the optical conductor line and the optical conductor line, an analyzer provided at the output end of the optical conductor line, a light receiving element for converting the output signal of the analyzer into an electrical signal, and a demodulating element for the light receiving element. a receiving side device consisting of a receiver connected via a transmitter, a transmitter, and an optical modulator connected to the transmitter via a modulator and optically modulating linearly polarized light propagating through the optical conductor line. a side device, the linearly polarized light propagating through the optical conductor line is optically modulated by the signal transmitted from the transmitting side device, and the optically modulated modulation component is detected and received by the receiving side device. It is expressed as a percentage.
〈実施例〉
本発明による通信装置を一実施例について図面を参照し
ながら説明する。<Embodiment> An embodiment of a communication device according to the present invention will be described with reference to the drawings.
第1図は本発明による通信装置の一実施例の構成図であ
る。第1図において、lは光変調効果を有する光導体線
路としての光ファイバ、2は光源、3は偏光子、4は検
光子、5は受光素子、6は復調器、7は受信器、8は移
動体、9は送信器、10は変調器、11は光変調器を構
成する電磁石である。本発明による通信装置に用いられ
る光ファイバは特に磁気光学効果の大きい光ファイバ例
えばヴエルデ常数が大きい常磁性ガラス例えば保谷硝子
社製FR−5(商品名)等をコアに用いた光ファイバが
適している。FIG. 1 is a block diagram of an embodiment of a communication device according to the present invention. In FIG. 1, l is an optical fiber as a light guide line having a light modulation effect, 2 is a light source, 3 is a polarizer, 4 is an analyzer, 5 is a light receiving element, 6 is a demodulator, 7 is a receiver, and 8 9 is a moving body, 9 is a transmitter, 10 is a modulator, and 11 is an electromagnet constituting an optical modulator. The optical fiber used in the communication device according to the present invention is particularly suitable for an optical fiber having a large magneto-optic effect, such as an optical fiber whose core is made of paramagnetic glass having a large Werde constant, such as FR-5 (trade name) manufactured by Hoya Glass Co., Ltd. There is.
又光ファイバの代りに磁気光学効果の大きいB S O
(Bit Sit O!oの結晶)あるいはZn5eの
素子を棒状にして配列した光導体線路でもよい。Also, instead of optical fiber, BSO has a large magneto-optic effect.
(Bit Sit O!o crystal) or a photoconductor line in which Zn5e elements are arranged in a rod shape.
本発明による通信装置によれば、図面に示す如く、光フ
ァイバlの入力端に入る光源2からの光は、偏光子3に
よって直線偏光される。この直線偏波光は光ファイバl
へ入力され、直線偏波面を保って光フアイバ内を伝搬す
る。また光ファイバlの出力端に置かれた検光子4は光
フアイバ1中を搬送する直線偏波光と直交する偏波面に
そって置かれている。−1移動体8上の送信器9から出
力された信号は変調器10を経て電磁石11を励振し、
励振磁界は光ファイバlと結合し、直線偏波光が伝搬す
る方向と同じ向きに加えられることによって偏波面が回
転する。回転角をθとすると、
θ=VH1!
V:グエルデ常数、
H:励振磁界の磁界の強さ。According to the communication device according to the present invention, the light from the light source 2 entering the input end of the optical fiber 1 is linearly polarized by the polarizer 3, as shown in the drawing. This linearly polarized light is transmitted through optical fiber l.
is input into the optical fiber, and propagates within the optical fiber while maintaining the linear polarization plane. Further, the analyzer 4 placed at the output end of the optical fiber 1 is placed along a polarization plane orthogonal to the linearly polarized light carried in the optical fiber 1. -1 The signal output from the transmitter 9 on the moving body 8 passes through the modulator 10 and excites the electromagnet 11,
The excitation magnetic field is coupled to the optical fiber 1 and applied in the same direction as the propagation direction of the linearly polarized light, thereby rotating the plane of polarization. If the rotation angle is θ, then θ=VH1! V: Guelde constant, H: magnetic field strength of excitation magnetic field.
l:伝搬路への励振磁界の作用区間長、である。光ファ
イバlの出力端に設けられた検光子4によって偏向成分
が検出され、受光索子5によって電気信号に変換され、
次いで復調器6で復調され、受信器7で信号が出力され
る。l: length of action section of the excitation magnetic field on the propagation path. A deflection component is detected by an analyzer 4 provided at the output end of the optical fiber l, and converted into an electrical signal by a light receiving probe 5.
Next, the demodulator 6 demodulates the signal, and the receiver 7 outputs the signal.
なお、信号形態はアナログ信号でもデジタル信号でもよ
く、変調方式もAM、FM、PCM等目的に応じて使用
できる。Note that the signal format may be an analog signal or a digital signal, and the modulation method may be AM, FM, PCM, etc. depending on the purpose.
以上は磁気光学効果を利用した光変調方式であるが、電
気光学効果を利用しても同様に光変調することができる
。電気光学効果を利用する光変調器の場合は、第1図に
示す電磁石の代りに第2図に示すような電極12a、1
2bが変調器lOに負荷される。尚電極12a、j2b
は光導体線路を間に挾んで変調信号電圧による電界が光
導体線路に印加され、光導体線路中を伝搬する直線偏波
光の偏波面を回転する。検光子4は光変調された成分を
検出し、受光素子5によって電気信号に変換し、受信機
7によって受信信号として出力する。Although the above is a light modulation method that uses the magneto-optic effect, it is also possible to similarly modulate light using the electro-optic effect. In the case of an optical modulator that utilizes the electro-optic effect, electrodes 12a, 1 as shown in FIG. 2 are used instead of the electromagnet shown in FIG.
2b is loaded onto the modulator lO. Note that the electrodes 12a, j2b
An electric field due to a modulated signal voltage is applied to the photoconductor line with the photoconductor line in between, thereby rotating the plane of polarization of the linearly polarized light propagating in the photoconductor line. The analyzer 4 detects the optically modulated component, converts it into an electrical signal by the light receiving element 5, and outputs it as a received signal by the receiver 7.
〈発明の効果〉
本発明による通信装置によれば送信側装置から受信側装
置へ、光導体線路を介して一方向通信ができるものであ
る。従来の誘導無線線路を用いたものに比較して、外来
雑音の影響がなく信号の質は極めて優れている。又線路
構造は簡単であり、線路の汚れに対し、本発明によるも
のはより影響を受けない点で勝れている。<Effects of the Invention> According to the communication device according to the present invention, one-way communication is possible from the transmitting side device to the receiving side device via the optical conductor line. Compared to conventional guided radio lines, the signal quality is extremely superior as there is no influence from external noise. Furthermore, the line structure is simple, and the line according to the present invention is superior in that it is less affected by dirt on the line.
第1図は本発明による通信装置の一実施例の構成図、第
2図は本発明による通信装置において電気光学効果を利
用した場合の光フアイバ励振用電極の構造を示す構成図
である。
図面中、
lは光ファイバ、
2は光源、
3は偏光子、
4は検光子、
5は受光素子、
6は復調器、
7は受信機、
8は移動体、
9は送信機、
lOは変調器、
11は電磁石、
12a、12bは電極である。FIG. 1 is a block diagram of an embodiment of a communication device according to the present invention, and FIG. 2 is a block diagram showing the structure of an electrode for excitation of an optical fiber when an electro-optic effect is utilized in a communication device according to the present invention. In the drawing, l is an optical fiber, 2 is a light source, 3 is a polarizer, 4 is an analyzer, 5 is a light receiving element, 6 is a demodulator, 7 is a receiver, 8 is a mobile object, 9 is a transmitter, and 1O is a modulator 11 is an electromagnet, and 12a and 12b are electrodes.
Claims (1)
に設けられた光源、該光源の光を直線偏光する上記光源
と光導体線路入力端の間に設けられた偏光子、上記光導
体線路の出力端に設けられた検光子、該検光子の検出出
力を電気信号に変換する受光素子並びに、該受光素子に
復調器を介して接続された受信機からなる受信側装置と
、送信機並びに、該送信機に変調器を介して接続され上
記光導体線路を伝搬する直線偏光を光変調する光変調器
からなる送信側装置とからなり、該送信側装置から発信
された信号によつて、上記光導体線路を伝搬する直線偏
光を光変調し、光変調された変調成分を上記受信側装置
によつて検出・受信することを特徴とする通信装置。A light guide line having a light modulation effect, a light source provided at the input end of the light guide line, a polarizer provided between the light source and the input end of the light guide line that linearly polarizes light from the light source, and the light guide line. A receiving side device consisting of an analyzer provided at the output end of the line, a light receiving element that converts the detection output of the analyzer into an electrical signal, and a receiver connected to the light receiving element via a demodulator, and a transmitter. and a transmitting side device consisting of an optical modulator connected to the transmitter via a modulator and optically modulating the linearly polarized light propagating through the optical conductor line, and by the signal transmitted from the transmitting side device. . A communication device, wherein the linearly polarized light propagating through the optical conductor line is optically modulated, and the optically modulated modulation component is detected and received by the receiving side device.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP59270707A JPS61148929A (en) | 1984-12-24 | 1984-12-24 | Communication device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP59270707A JPS61148929A (en) | 1984-12-24 | 1984-12-24 | Communication device |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS61148929A true JPS61148929A (en) | 1986-07-07 |
Family
ID=17489837
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP59270707A Pending JPS61148929A (en) | 1984-12-24 | 1984-12-24 | Communication device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS61148929A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
FR2619909A1 (en) * | 1987-08-27 | 1989-03-03 | Comp Generale Electricite | Device for incremental measurement of a linear displacement |
-
1984
- 1984-12-24 JP JP59270707A patent/JPS61148929A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
FR2619909A1 (en) * | 1987-08-27 | 1989-03-03 | Comp Generale Electricite | Device for incremental measurement of a linear displacement |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
JP2791856B2 (en) | Electric field sensor | |
US7809216B2 (en) | Bi-directional signal interface and apparatus using same | |
US5015053A (en) | Reduction of modulator non-linearities with independent bias angle control | |
EP0758090A3 (en) | An electromagnetic wave-to-optical signal converting and modulating device and a communication system using the same | |
EP0287379B1 (en) | Transmission system | |
WO2009131916A2 (en) | Bi-directional signal interface with enhanced isolation | |
EP1348993B1 (en) | Magneto-optic modulator and optical communication system using the same | |
US10790911B2 (en) | Modified Sagnac loop coherent phase modulated RF photonic link | |
JPS61148929A (en) | Communication device | |
US6490070B1 (en) | Method and apparatus for polarization tracking in wireless optical communication systems | |
EP0630121A1 (en) | Apparatus and method employing fast polarization modulation to reduce effects of polarization hole burning and/or polarization dependent loss | |
JP2760856B2 (en) | Phase shift keying method using Mach-Zehnder type optical modulator | |
CN105634731B (en) | The magneto-optic acousto-optic joint coding method of single spatial mode coherent light communication | |
AU690181B2 (en) | An optical communications system having a polarization scrambler | |
US20200333405A1 (en) | Optical probe system and method | |
JP3435588B2 (en) | Electric field sensor | |
JPH1075216A (en) | Light amplifier type optical communication system for changing gain by polarization of input signal | |
JP2021196203A (en) | Optical electric field sensor head | |
JP2768787B2 (en) | Optical communication method | |
RU67297U1 (en) | DEVICE FOR MODULATION AND DETECTION OF OPTICAL RADIATION | |
JP2562287Y2 (en) | Electric field antenna | |
JP3505669B2 (en) | Electric field sensor | |
JPH0829467A (en) | Electric field sensor | |
JP2003258723A (en) | Radio wave reception / optical transmission system | |
JPH06164498A (en) | Optical transmitter and optical modulation device using for the same |