JPS6239860B2 - - Google Patents
Info
- Publication number
- JPS6239860B2 JPS6239860B2 JP56153970A JP15397081A JPS6239860B2 JP S6239860 B2 JPS6239860 B2 JP S6239860B2 JP 56153970 A JP56153970 A JP 56153970A JP 15397081 A JP15397081 A JP 15397081A JP S6239860 B2 JPS6239860 B2 JP S6239860B2
- Authority
- JP
- Japan
- Prior art keywords
- output
- interference
- received signal
- signal
- polarization
- 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.)
- Expired
Links
- 230000010287 polarization Effects 0.000 claims description 17
- 230000002452 interceptive effect Effects 0.000 claims description 7
- 230000005540 biological transmission Effects 0.000 description 6
- 238000004891 communication Methods 0.000 description 6
- 238000010586 diagram Methods 0.000 description 6
- 238000005388 cross polarization Methods 0.000 description 5
- 230000008878 coupling Effects 0.000 description 2
- 238000010168 coupling process Methods 0.000 description 2
- 238000005859 coupling reaction Methods 0.000 description 2
- 238000005516 engineering process Methods 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 230000006866 deterioration Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 239000004615 ingredient Substances 0.000 description 1
- 230000010354 integration Effects 0.000 description 1
- 238000010295 mobile communication Methods 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04B—TRANSMISSION
- H04B7/00—Radio transmission systems, i.e. using radiation field
- H04B7/002—Reducing depolarization effects
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04L—TRANSMISSION OF DIGITAL INFORMATION, e.g. TELEGRAPHIC COMMUNICATION
- H04L27/00—Modulated-carrier systems
- H04L27/02—Amplitude-modulated carrier systems, e.g. using on-off keying; Single sideband or vestigial sideband modulation
- H04L27/06—Demodulator circuits; Receiver circuits
Landscapes
- Engineering & Computer Science (AREA)
- Computer Networks & Wireless Communication (AREA)
- Signal Processing (AREA)
- Digital Transmission Methods That Use Modulated Carrier Waves (AREA)
Description
【発明の詳細な説明】
この発明は、無線伝送の直交偏波共用にともな
い生じる交差偏波干渉補償技術に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a technology for compensating for cross-polarization interference that occurs when orthogonal polarizations are shared in wireless transmission.
マイクロ波帯の無線通信は地上通信並びに衛星
通信を中心に急速に発展している。無線通信の需
要は今後移動通信サービスの拡大等の理由で更に
増大していくことが予想され、準ミリ波以上の周
波数帯開拓と共に、実用的価値の高い現用の周波
数帯のいわゆる周波数再利用の考えが高まつてい
る。 Microwave band wireless communications are rapidly developing, centering on terrestrial communications and satellite communications. The demand for wireless communications is expected to further increase in the future due to the expansion of mobile communication services, etc., and along with the development of sub-millimeter wave and higher frequency bands, so-called frequency reuse of currently used frequency bands with high practical value is expected. Thoughts are growing.
本来、自由空間は直交する2偏波に対して独立
で、両偏波を同時に伝送できる伝送線路である
が、実際の伝搬路には降雨などの媒質の異方性が
存在し、直交偏波共用方式を採用すると、交差偏
波の発生による偏波間の結合が異偏波チヤンネル
干渉を起すことになる。 Originally, free space is independent of two orthogonal polarized waves, and is a transmission line that can simultaneously transmit both polarized waves. However, in actual propagation paths, there is anisotropy in media such as rain, and orthogonal polarized waves If a shared system is adopted, coupling between polarized waves due to the generation of cross-polarized waves will cause interference between different polarization channels.
従つて、直交偏波共用化の達成には、アンテナ
や給電装置などの偏波特性の改善と共に降雨など
による電波伝搬上の偏波特性の劣化を補償する交
差偏波補償回路の開発も重要な課題となつてい
る。 Therefore, in order to achieve cross-polarization sharing, it is necessary to improve the polarization characteristics of antennas and power supply equipment, as well as develop a cross-polarization compensation circuit that compensates for the deterioration of polarization characteristics during radio wave propagation due to rain, etc. This has become an important issue.
交差偏波補償技術は、かかる偏波間の結合をア
ンテナ給電装置や無線機器内に補償回路を設けて
自動的な補償を行なうものである。 Cross polarization compensation technology automatically compensates for such coupling between polarized waves by providing a compensation circuit within an antenna feeder or wireless device.
従来、マイクロ波帯通信はFMを中心とするア
ナログ伝送が中心であつたが、近年、マイクロ波
帯においても、デイジタル伝送が使用される様に
なり交差偏波補償方式についてもデイジタル伝送
の特徴を生かしたより効率の良い方式の提案が要
請されている。 Conventionally, microwave band communication has centered on analog transmission, mainly FM, but in recent years, digital transmission has come to be used in the microwave band as well, and cross-polarization compensation methods have also adopted the characteristics of digital transmission. Proposals for more efficient methods are requested.
従来、この種の回路は、相互に直交する2つの
偏波を受信し、一方(干渉側)の受信信号に補償
係数を乗じて他方(受信希望側)の受信信号から
減ずることによつて干渉成分を除去するようにし
ている。例えば、水平偏波と垂直偏波とを考え、
各々に独立なデータH、Vを乗せると、伝播中に
生じた偏波干渉αV、βHにより、水平偏波の受
信信号H0および垂直偏波の受信信号V0は、
H0=H+αV ……(1)
V0=V+βH ……(2)
となる。今、データHを受信したい場合を考える
と、垂直偏波の受信信号V0に補償係数Ωを乗じ
て水平受信信号H0に加えて干渉除去信号Heを得
るようにするのが一般的である。すなわち、
He=H0+ΩV0 ……(3)
従つて、
He=H+αV+Ω(V+βH)=H+(α+Ω)
V
+Ω・β・H≒H+(α+Ω)V ……(4)
すなわち、α=−Ωとすることによつて
He≒H ……(5)
となり、偏波干渉が除去される。このときΩの制
御は、一般に
Ω(i+1)=Ω(i)−kV0 *・(He−H^e) ……(6)
となるように制御される。ここにH^eはHeの識
別値であり、He−H^eは識別誤差eであつて垂
直偏波からの干渉が含まれている。従つてeと
V0との相関を最小化する方向にΩを制御すれ
ば、α=−Ωとなり、干渉が除去されることにな
る。 Conventionally, this type of circuit receives two mutually orthogonal polarized waves, multiplies the received signal of one (interfering side) by a compensation coefficient, and subtracts it from the received signal of the other (desired side) to eliminate interference. We are trying to remove the ingredients. For example, considering horizontal polarization and vertical polarization,
When independent data H and V are placed on each, due to the polarization interference αV and βH that occurred during propagation, the horizontally polarized received signal H 0 and the vertically polarized received signal V 0 become H 0 = H + αV... (1) V 0 =V+βH ...(2) Now, if we consider the case where we want to receive data H, it is common to multiply the vertically polarized received signal V0 by a compensation coefficient Ω to obtain the interference cancellation signal He in addition to the horizontal received signal H0 . . That is, He=H 0 +ΩV 0 ...(3) Therefore, He=H+αV+Ω(V+βH)=H+(α+Ω)
V +Ω・β・H≈H+(α+Ω)V (4) That is, by setting α=−Ω, He≈H (5), and polarization interference is removed. At this time, Ω is generally controlled so that Ω (i+1) = Ω (i) −kV 0 * ·(He−H^e) (6). Here, H^e is the discrimination value of He, and He-H^e is the discrimination error e, which includes interference from vertically polarized waves. Therefore, e and
If Ω is controlled in a direction that minimizes the correlation with V 0 , α=−Ω, and interference will be removed.
しかし、V0 *・eは複素乗算であつて、高価
なアナログ乗算器を必要とし、特に伝送レートが
高速の場合は非常に高価である。 However, V 0 * ·e is a complex multiplication and requires an expensive analog multiplier, which is very expensive especially when the transmission rate is high.
本発明の目的は、上述の従来の欠点を解消し、
複素乗算器を使用しないで、上記V0 *・eに比
例する値を得ることができる安価な偏波干渉除去
回路を提供することにある。 The object of the present invention is to overcome the above-mentioned conventional drawbacks and to
The object of the present invention is to provide an inexpensive polarization interference cancellation circuit that can obtain a value proportional to the above V 0 * ·e without using a complex multiplier.
本発明の干渉除去回路は、相互に直交する2つ
の偏波を受信し、一方の受信信号に補償係数を乗
じて他方の受信信号に加えることにより偏波干渉
成分を除去する偏波干渉除去回路において、補償
後の受信信号とその識別値との誤差を検出する識
別誤差検出器と、干渉側受信信号の実質成分と虚
数成分がいずれも正であつて大きさが等しいとき
に出力する干渉側識別器と、前記識別誤差検出器
の出力値の実数成分と虚数成分との和および差を
出力する加算器および減算器と、該加算器および
減算器の出力を前記干渉側識別器の出力によつて
導通させる開閉器と、該開閉器の出力を平滑して
前記補償係数を出力する低域波器とを備えたこ
とを特徴とする。 The interference cancellation circuit of the present invention receives two mutually orthogonal polarized waves, multiplies one received signal by a compensation coefficient, and adds it to the other received signal to remove the polarization interference component. , an identification error detector that detects the error between the compensated received signal and its identification value, and an interference side that outputs when the real component and imaginary component of the interference side reception signal are both positive and equal in magnitude. a discriminator, an adder and a subtracter that output the sum and difference between the real component and the imaginary component of the output value of the discrimination error detector, and outputs of the adder and subtracter as outputs of the interference side discriminator. The present invention is characterized in that it includes a switch that conducts through the switch, and a low frequency generator that smoothes the output of the switch and outputs the compensation coefficient.
次に、本発明について、図面を参照して詳細に
説明する。 Next, the present invention will be explained in detail with reference to the drawings.
先ず、本発明の原理について説明する。今、受
信信号V0の実数部をVR、虚数部VI、識別誤差
信号eの実数部をeR、虚数部eIとすると、
V0=VR+jVI ……(7)
e=eR+jeI ……(8)
であるから、
V0 *e=(VR−jVI)(eR+jeI)
=(VReR+VIeI)+j(VReI−VIeR)
である。ここで、
VR=VI>0 ……(9)
の時は、
V0 *e∝(eR+eI)j(eI−eR) ……(10)
となるから、上記(10)式は加算器のみで求めること
ができる。すなわち、本発明は、(9)式を満足する
時にのみ(10)式の値を出力させ、これによつて補償
係数を制御することにより干渉波成分を除去する
ものである。 First, the principle of the present invention will be explained. Now, if the real part of the received signal V 0 is VR , the imaginary part V I , the real part of the identification error signal e is e R , and the imaginary part e I , then V 0 = VR + jV I ...(7) e= E _ _ _ _ _ _ _ _ _ _ _ _ _ IeR ) . Here, when VR = V I > 0 ... (9), V 0 * e∝ (e R + e I ) j (e I − e R ) ... (10), so the above (10 ) can be obtained using only an adder. That is, the present invention removes the interference wave component by outputting the value of equation (10) only when equation (9) is satisfied, and thereby controlling the compensation coefficient.
例えば、第1図に示すような16値振幅位相変調
(16QAM)の信号のうち、黒丸印の信号は(9)式を
満足している。 For example, among the 16-level amplitude phase modulation (16QAM) signals shown in FIG. 1, the signals marked with black circles satisfy equation (9).
第2図は、(9)式を満足するとき出力信号を出す
ようにした干渉側識別器の一例を示す回路図であ
る。すなわち、端子300,301へは、干渉側
受信信号の実数部VRおよび虚数部VIがそれぞれ
入力し、減算器31で減算し、折返し回路32で
差の絶対値を出力し、比較回路33で比較するこ
とにより|VR|≒|VI|が検出される。VR>
0は比較器30で検出される。比較器30と34
の両出力はアンド回路34で論理積がとられて出
力端子302に出力される。 FIG. 2 is a circuit diagram showing an example of an interference side discriminator that outputs an output signal when formula (9) is satisfied. That is, the real part V R and the imaginary part V I of the interfering side reception signal are respectively input to the terminals 300 and 301, subtracted by the subtracter 31, outputted as the absolute value of the difference by the folding circuit 32, and then outputted by the comparator circuit 33. |V R |≒|V I | is detected by comparing. V R >
0 is detected by comparator 30. Comparators 30 and 34
Both outputs are ANDed by an AND circuit 34 and output to an output terminal 302.
第3図は、本発明の一実施例を示すブロツク図
である。すなわち、偏波干渉減算回路6の入力端
子600に例えば水平偏波受信信号H0を入力さ
せ、入力端子601には垂直偏波受信信号V0を
入力させる。垂値偏波受信信号V0は乗算器61
で補償係数Ωが乗ぜられて加算器60において水
平偏波受信信号H0に加えられる。従つて出力端
子602には、干渉除去信号Heが出力する。す
なわち(3)式が実現される。干渉除去信号Heは、
識別誤差検出器1の入力端子100に接続され、
識別器10によつて識別値H^eが出力され、減算
器11によつて前記Heとの差がとられて識別誤
差eが端子101から出力する。識別誤差eの実
数部eRと虚数部eIは、相関器2の内蔵する加算
器22によつて加算され、減算器23によつて減
算される。加算器22の出力は、(10)式右辺の(e
R+eI)を与え、減算器23の出力は(10)式右辺の
(eR−eI)を与えている。これらの出力は開閉
器4(スイツチ40,41)が閉じたときにそれ
ぞれ積分器50および51に供給され、(6)式に示
した積分動作が行なわれ、平滑化される。開閉器
4は干渉側識別器3の出力によつて閉じる開閉器
であり、干渉側識別器3は、前述の第2図に示す
ように構成されていて、(9)式を満足するときのみ
出力を出す。従つて、開閉器4は(9)式が満足され
るときだけ導通するから、このときの相関器2の
出力は、(10)式により前記V0 *eに比例する。加算
器22の出力は積分器50によつて平滑化されて
補償係数Ωの実数部ΩRとされ、減算器23の出
力は、積分器51によつて平滑化されて補償係数
Ωの虚数部ΩIとされる。積分器50,51で複
素低域波器50を構成している。すなわち、(6)
式のΩを乗算器を用いないで得ることができる。
上記補償係数Ωは前述の通り乗算器61によつて
垂直偏波受信信号V0に乗ぜられて水平偏波受信
信号H0に加えられることにより偏波干渉が打消
される。補償残りは、識別誤差信号eとなつて上
述の動作により次の補償係数を補正する。 FIG. 3 is a block diagram showing one embodiment of the present invention. That is, for example, the horizontally polarized received signal H 0 is input to the input terminal 600 of the polarization interference subtraction circuit 6, and the vertically polarized received signal V 0 is inputted to the input terminal 601. The vertical polarization received signal V 0 is sent to the multiplier 61
is multiplied by a compensation coefficient Ω and added to the horizontally polarized received signal H 0 in an adder 60 . Therefore, the interference cancellation signal He is output to the output terminal 602. In other words, equation (3) is realized. The interference cancellation signal He is
connected to the input terminal 100 of the identification error detector 1;
The discriminator 10 outputs the discrimination value H^e, the subtracter 11 calculates the difference from the above He, and the discrimination error e is output from the terminal 101. The real part e R and the imaginary part e I of the identification error e are added by an adder 22 built in the correlator 2 and subtracted by a subtracter 23 . The output of the adder 22 is (e
R +e I ) is given, and the output of the subtracter 23 gives (e R −e I ) on the right side of equation (10). These outputs are supplied to integrators 50 and 51, respectively, when the switch 4 (switches 40, 41) is closed, and are subjected to the integration operation shown in equation (6) and smoothed. The switch 4 is a switch that is closed by the output of the interference side discriminator 3, and the interference side discriminator 3 is configured as shown in FIG. Give output. Therefore, since the switch 4 becomes conductive only when the equation (9) is satisfied, the output of the correlator 2 at this time is proportional to the V 0 * e according to the equation (10). The output of the adder 22 is smoothed by an integrator 50 to become the real part Ω R of the compensation coefficient Ω, and the output of the subtracter 23 is smoothed by the integrator 51 to become the imaginary part of the compensation coefficient Ω. Ω I. Integrators 50 and 51 constitute a complex low-pass filter 50. That is, (6)
Ω in the equation can be obtained without using a multiplier.
As described above, the compensation coefficient Ω is multiplied by the vertically polarized received signal V 0 by the multiplier 61 and added to the horizontally polarized received signal H 0 to cancel polarization interference. The remaining compensation becomes the identification error signal e, and the next compensation coefficient is corrected by the above-described operation.
また、干渉側識別器の出力する条件は(9)式に限
らず、|VR|=|VI|を満足する信号の検出を
行ない、V0の属する象限によつて相関器の極性
を変えるようにしても良い。 In addition, the condition for the output of the interfering side discriminator is not limited to equation (9); it also detects a signal that satisfies |V R |= |V I |, and determines the polarity of the correlator depending on the quadrant to which V 0 belongs. You may try changing it.
以上のように、本発明においては、干渉側偏波
信号に補償係数を乗じて受信希望側の信号に加え
ることによつて干渉除去信号を得、該干渉除去信
号と識別信号との差、すなわち識別誤差信号の実
数部と虚数部の和および差の信号によつて、干渉
側信号が一定の条件を満足するときにのみ補償係
数を修正するように構成されているから、乗算器
を用いないで補償係数を最適、かつ自動的に変化
させることができる。すなわち、良好な干渉波除
去信号を得ることができ受信データ品質が向上す
るという効果がある。本発明によれば、衛星通信
における宇宙空間のフアラデー・ローテーシヨン
による偏波干渉変化に対しても迅速かつ精確に追
従できる。 As described above, in the present invention, an interference cancellation signal is obtained by multiplying the interfering side polarized signal by a compensation coefficient and adding it to the signal on the receiving side, and the difference between the interference cancellation signal and the identification signal, i.e. Since the system is configured to modify the compensation coefficient only when the interfering signal satisfies certain conditions using the sum and difference signals of the real and imaginary parts of the identification error signal, no multiplier is used. The compensation coefficient can be changed optimally and automatically. That is, there is an effect that a good interference wave cancellation signal can be obtained and the quality of received data is improved. According to the present invention, it is possible to quickly and accurately follow changes in polarization interference due to Faraday rotation in outer space in satellite communications.
第1図は16値振幅位相変調信号の各信号点およ
び特定の条件を満たす信号点を示す図、第2図は
本発明に使用する干渉側識別器の一例を示す回路
図、第3図は本発明の一実施例を示すブロツク図
である。
図において、1……識別誤差検出器、2……相
関器、3……干渉側識別器、4……開閉器、5…
…低域波器、6……偏波干渉減算回路、10…
…識別器、11……減算器、22……加算器、2
3……減算器、30,33……比較器、31……
減算器、32……折返し回路、34……アンド回
路、40,41……開閉器、50,51……積分
器、60……加算器、61……乗算器。
Fig. 1 is a diagram showing each signal point of a 16-level amplitude phase modulation signal and signal points that satisfy specific conditions, Fig. 2 is a circuit diagram showing an example of an interference side discriminator used in the present invention, and Fig. 3 is a diagram showing signal points that satisfy specific conditions. FIG. 1 is a block diagram showing one embodiment of the present invention. In the figure, 1...Identification error detector, 2...Correlator, 3...Interfering side discriminator, 4...Switch, 5...
...Low frequency filter, 6...Polarization interference subtraction circuit, 10...
... Discriminator, 11 ... Subtractor, 22 ... Adder, 2
3...Subtractor, 30, 33...Comparator, 31...
Subtractor, 32... folding circuit, 34... AND circuit, 40, 41... switch, 50, 51... integrator, 60... adder, 61... multiplier.
Claims (1)
受信信号に補償係数を乗じて他方の受信信号に加
えることにより偏波干渉成分を除去する偏波干渉
除去回路において、補償後の受信信号とその識別
値との誤差を検出する識別誤差検出器と、干渉側
受信信号の実数成分と虚数成分がいずれも正であ
つて大きさが等しいときに出力する干渉側識別器
と、前記識別誤差検出器の出力値の実数成分と虚
数成分との和および差を出力する加算器および減
算器と、該加算器および減算器の出力を前記干渉
側識別器の出力によつて導通させる開閉器と、該
開閉器の出力を平滑して前記補償係数を出力する
低域波器とを備えたことを特徴とする偏波干渉
除去回路。1 In a polarization interference removal circuit that receives two mutually orthogonal polarized waves and removes the polarization interference component by multiplying one received signal by a compensation coefficient and adding it to the other received signal, the received signal after compensation is an interference side discriminator that outputs an error when both the real component and the imaginary component of the interfering side received signal are positive and equal in magnitude; an adder and a subtracter that output the sum and difference between the real component and the imaginary component of the output value of the detector; and a switch that connects the output of the adder and subtracter with the output of the interference side discriminator. , and a low frequency device that smoothes the output of the switch and outputs the compensation coefficient.
Priority Applications (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56153970A JPS5856544A (en) | 1981-09-30 | 1981-09-30 | Eliminating circuit for polarized wave interference |
| US06/416,112 US4479258A (en) | 1981-09-30 | 1982-09-09 | Cross-polarization crosstalk canceller |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56153970A JPS5856544A (en) | 1981-09-30 | 1981-09-30 | Eliminating circuit for polarized wave interference |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5856544A JPS5856544A (en) | 1983-04-04 |
| JPS6239860B2 true JPS6239860B2 (en) | 1987-08-25 |
Family
ID=15574050
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP56153970A Granted JPS5856544A (en) | 1981-09-30 | 1981-09-30 | Eliminating circuit for polarized wave interference |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5856544A (en) |
-
1981
- 1981-09-30 JP JP56153970A patent/JPS5856544A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5856544A (en) | 1983-04-04 |
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