JPS6016761B2 - Detection device for all carrier single sideband signals - Google Patents
Detection device for all carrier single sideband signalsInfo
- Publication number
- JPS6016761B2 JPS6016761B2 JP10826476A JP10826476A JPS6016761B2 JP S6016761 B2 JPS6016761 B2 JP S6016761B2 JP 10826476 A JP10826476 A JP 10826476A JP 10826476 A JP10826476 A JP 10826476A JP S6016761 B2 JPS6016761 B2 JP S6016761B2
- Authority
- JP
- Japan
- Prior art keywords
- signal
- single sideband
- detection device
- amplitude
- phase
- 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
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- Digital Transmission Methods That Use Modulated Carrier Waves (AREA)
Description
【発明の詳細な説明】
本発明は全搬送波を送出する単側帯波振幅変調・信号を
再生検波する装置に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an apparatus for reproducing a single sideband amplitude modulated signal that transmits a full carrier wave.
単側帯波振幅変調信号(以下SSB−AM信号と記す)
の検波方式として同期検波方式がよく知られている。即
ち第1図に示すように原理的には送信側において入力情
報Siは周波数変換器1において局部周波数源3からの
局部搬送波により周波数変換され、その一方の側帯波が
送信される。受信信号は送信側局部周波数源3の発振周
波数と極めて近い発振周波数を有する局部周波数源4か
らの局部搬送波と周波数変換器2で周波数混合され、情
報信号力Soとして再生される。このように従来におい
ては受信信号は周波数変換されることによって情報信号
にかえられるため、SSB−AM信号の大気中伝搬の際
に受けるフェージングの影響などによる受信電界強度の
変動が直接的に情報信号の雑音となる欠点があった。本
発明は搬送波を送出するSSB−AM信号、いわゆる全
搬送波SSB一AM信号の大気中伝搬におけるフェージ
ングの影響を受けにくい位相変調成分から情報信号を検
出することを特徴とし、その目的はSSB−AM無線通
信方式の伝送品質を改善することにある。Single sideband amplitude modulation signal (hereinafter referred to as SSB-AM signal)
The synchronous detection method is well known as a detection method for this. That is, as shown in FIG. 1, in principle, on the transmitting side, input information Si is frequency-converted by a frequency converter 1 using a local carrier wave from a local frequency source 3, and one of the sidebands is transmitted. The received signal is frequency-mixed by the frequency converter 2 with a local carrier wave from a local frequency source 4 having an oscillation frequency very close to the oscillation frequency of the transmitting local frequency source 3, and is reproduced as an information signal power So. Conventionally, the received signal is converted into an information signal by frequency conversion, so fluctuations in the received electric field strength due to the effects of fading during atmospheric propagation of the SSB-AM signal directly affect the information signal. The problem was that it caused noise. The present invention is characterized in that an information signal is detected from a phase modulation component that is less susceptible to fading in the atmospheric propagation of an SSB-AM signal that transmits a carrier wave, a so-called all-carrier SSB-AM signal. The objective is to improve the transmission quality of wireless communication systems.
この発明による全搬送波SSB−AM信号の検波装置の
原理をまず説明する。First, the principle of the all-carrier SSB-AM signal detection device according to the present invention will be explained.
一般に全搬送波上側帯波SSB一AM信号es(t)は
eS(t)=Re〔(C十S(t)十iH〔S(t)〕
)ejのct〕 ,..(1)
=R(t)Re〔ejwqei○(t)〕 …■で与
えられる。Generally, the total carrier upper sideband SSB-AM signal es(t) is eS(t)=Re[(C0S(t)1iH[S(t)]
) ej ct] ,. .. (1)
=R(t)Re[ejwqei○(t)] ...■.
ただしC:正の定数、S(t):情報信号、C+S(t
)>0,日〔S(t)〕:S(t)のヒルベルト変換、
のc:搬送波の角周波数、R(t)= {(C+S(t
))2 十日2〔S(t)〕}1′2,◇(t)=ねn
−・〔聖書器号〕,Re:実数成分をそれぞれ意味する
。However, C: positive constant, S(t): information signal, C+S(t
) > 0, day [S(t)]: Hilbert transform of S(t),
c: angular frequency of carrier wave, R(t) = {(C+S(t
))2 10 days 2 [S(t)]}1'2, ◇(t)=ne n
-・[Bible name], Re: Each means a real number component.
情報信号S(t)と包絡線R(t)および位相変調成分
?(t)との関係は次式で与えられる。Information signal S(t), envelope R(t) and phase modulation component? The relationship with (t) is given by the following equation.
C+S(t)=R(t)COS?(t) …(31
また包絡線R(t)と位送変調成分0(t)とはつぎの
関係が成立することが知られている。つくt)=日〔l
n(R(t)/C〕 …【4,R(t)/C=e‐
日〔つ(t)〕 …■この関係を利用して第
【3}式は・十響=e‐日〔小〕xCOS◇(t).・
・【6’とかき換えられる。C+S(t)=R(t)COS? (t) …(31
It is also known that the following relationship holds between the envelope R(t) and the phase modulation component 0(t). t) = day [l
n(R(t)/C]...[4,R(t)/C=e-
Day [tsu (t)] ...■Using this relationship, the formula [3} is: Ten Symphony = e - day [small] x COS◇ (t).・
・[Can be replaced with 6'.
この式は全搬送波SSB−AM信号の位相変調成分で(
t)から情報信号S(t)が再生できることを示してい
る。以上述べた原理に従って構成したこの発明の実施例
を第2図に示す。This formula is the phase modulation component of the total carrier SSB-AM signal (
This shows that the information signal S(t) can be reproduced from t). FIG. 2 shows an embodiment of the present invention constructed according to the principles described above.
受信された全搬送波SSB−AM信号は振幅制限器5に
よりその包絡線成分R(t)が除去されe,(t)とな
る。e,(t)=K,Re〔ejのCteJ○(t)〕
…【7}ただしK,は定数である。The envelope component R(t) of the received full carrier SSB-AM signal is removed by the amplitude limiter 5, resulting in e,(t). e, (t) = K, Re [CteJ○(t) of ej]
...[7} However, K is a constant.
このe,(t)より搬送波抽出回路6にて搬送波周波数
が抽出され、その搬送波は90o移相器7にて90o移
相されて周波数変換器2へ供給され、振幅制限器5の出
力e,(t)は直交同期検波されe2(t)が得られる
。e2(t)=K,K2Sin○(t)
…■ただしK2は定数である。K,K2=1に調整し
た後e2(t)は逆正弦関数器8に入力されてe2(t
)が逆正弦関数に変換され位相変調成分ぐ(t)が得ら
れる。つまりこの生力e3(t)はe3(t)=sin
‐1〔e2(t)〕=◇(t) …■となる。このよ
うにして取出された位相変調成分◇(t)は二分され、
その一方は広帯域900位相器1川こて900移相され
、指数関数器11にて指数関数に変換されて包絡線成分
R(t)に変換される。すなわちe4(t)=e‐日〔
ザ〕=学 ...(,。A carrier wave frequency is extracted by a carrier wave extracting circuit 6 from these e, (t), and the carrier wave is phase-shifted by 90 degrees by a 90 degree phase shifter 7 and supplied to the frequency converter 2, and the output of the amplitude limiter 5 is e, (t) is subjected to orthogonal synchronous detection to obtain e2(t). e2(t)=K,K2Sin○(t)
...■ However, K2 is a constant. After adjusting K, K2=1, e2(t) is input to the arc sine function unit 8 and becomes e2(t
) is converted into an inverse sine function to obtain a phase modulation component (t). In other words, this raw force e3(t) is e3(t)=sin
-1[e2(t)]=◇(t) ...■. The phase modulation component ◇(t) extracted in this way is divided into two,
One of them is phase-shifted by a wideband 900 phase shifter and 900 degrees, and is converted into an exponential function by an exponential function unit 11 and converted into an envelope component R(t). That is, e4(t) = e-day [
The = science. .. .. (,.
)が得られる。また二分された位相変調成分?(t)の
他方は余弦関数器9により糸弦関数がとられe5(t)
が得られる。e5(t)=K3cosつくt)
…(11)e4(t)及びe5(t)は乗算器1
2で乗算され、情報信号S(t)が再生される。) is obtained. Another bisected phase modulation component? The other of (t) is given a string function by the cosine function unit 9, and becomes e5(t).
is obtained. e5(t)=K3cos t)
...(11) e4(t) and e5(t) are multiplier 1
2 to reproduce the information signal S(t).
つまりe6(t)=e4(t)xe5(t)=K3掌C
OSo(t):さ(C+S(t)) ‐‐‐(12
)が縛られる。In other words, e6(t) = e4(t) xe5(t) = K3 palm C
OSo(t):Sa(C+S(t)) ---(12
) is bound.
第3図に周波数弁別器と積分器とにより位相変調成分0
(t)を検出する構成を示す。Figure 3 shows that the phase modulation component is zero due to the frequency discriminator and integrator.
A configuration for detecting (t) is shown.
振幅制限器5の出力e,(t)はのcを基準とした周波
数弁別器13にて周波数弁別され、その出力は位相変調
成分ぐ(t)の時間微分信号e7(t)となる。e7(
t)=K4つ′(t) …(13ただしK
4は定数である。e7(t)は積分器14によつてe8
(t)=K4&◇(t)十KB …(1心に
変換される。The output e,(t) of the amplitude limiter 5 is subjected to frequency discrimination by a frequency discriminator 13 using c as a reference, and its output becomes a time differential signal e7(t) of the phase modulation component g(t). e7(
t) = K4'(t) ...(13 but K
4 is a constant. e7(t) is converted to e8 by the integrator 14.
(t)=K4&◇(t) 10KB...(Converted to 1 core.
ここでK4&:1,K6=0に設定することによってe
8(t)=◇(t) …(15)
が得られる。Here, by setting K4&:1, K6=0, e
8(t)=◇(t)...(15)
is obtained.
このようにして得られたぐ(t)より第2図に示したと
同様にして情報信号S(t)が再生される。以上のよう
に本発明では受信信号をまず振幅制限処理するため、フ
ェージングなどの受信電界強度の変動による雑音の軽減
が可能となる。From the signal S(t) thus obtained, the information signal S(t) is reproduced in the same manner as shown in FIG. As described above, in the present invention, since the received signal is first subjected to amplitude limiting processing, it is possible to reduce noise caused by fluctuations in received electric field strength such as fading.
以上説明したように本発明は全搬送波SSB−AM信号
の位相変調成分から情報信号を再生するため受信系の最
前段に振幅制限器を使用でき、フヱージングなど伝搬の
際のレベル変動による雑音を軽減できる利点がある。As explained above, the present invention can use an amplitude limiter at the front stage of the receiving system to reproduce information signals from the phase modulation components of all carrier SSB-AM signals, thereby reducing noise caused by level fluctuations during propagation such as fading. There are advantages that can be achieved.
第1図は同期検波方式の単側帯波通信方式の原理を示す
ブロック図、第2図は本発明によるSSB−AM信号の
検波装置の実施例を示すブロック図、第3図は本発明に
よるSSB−AM信号の検波装置の他の例を示すブロッ
ク図である。
。1,2:周波数変換器、3,4:局部周波数源、5:
振幅制限器、6:搬送波抽出回路、7:9び移相器、8
:逆正弦関数器、9:余弦関数器、10:広帯域90o
移相器、11:指数関数器、12:乗算器、13:周波
数弁別器、14:積分器。
髪イ図
第2図
募る図FIG. 1 is a block diagram showing the principle of a single sideband communication system using a synchronous detection method, FIG. 2 is a block diagram showing an embodiment of an SSB-AM signal detection device according to the present invention, and FIG. 3 is a block diagram showing an embodiment of an SSB-AM signal detection device according to the present invention - It is a block diagram showing another example of the AM signal detection device. . 1, 2: Frequency converter, 3, 4: Local frequency source, 5:
Amplitude limiter, 6: Carrier extraction circuit, 7: Phase shifter, 8
: Arcsine function unit, 9: Cosine function unit, 10: Wideband 90o
Phase shifter, 11: Exponential function unit, 12: Multiplier, 13: Frequency discriminator, 14: Integrator. Hair diagram Figure 2 Recruitment diagram
Claims (1)
限する振幅制限器と、その振幅制限出力の位相成分を抽
出する手段と、その抽出された位相成分を90°移相す
る90°移相器と、その移相出力の指数関数をとつて包
絡線成分を再生する指数関数器と、上記抽出された位相
成分の余弦関数をとる余弦関数器と、その余弦関数出力
と、上記再生された包絡線成分との乗算により情報信号
の再生出力を得る乗算器とを具備する全搬送波単側帯波
信号の検波装置。1. An amplitude limiter for amplitude limiting a received all-carrier single sideband amplitude modulated signal, means for extracting a phase component of the amplitude-limited output, and a 90° phase shifter for shifting the extracted phase component by 90°. an exponential function generator that takes the exponential function of its phase shift output to reproduce the envelope component, a cosine function function that takes the cosine function of the phase component extracted above, the cosine function output, and the above reproduced 1. A detection device for an all-carrier single sideband signal, comprising a multiplier that obtains a reproduced output of an information signal by multiplication with an envelope component.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10826476A JPS6016761B2 (en) | 1976-09-08 | 1976-09-08 | Detection device for all carrier single sideband signals |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10826476A JPS6016761B2 (en) | 1976-09-08 | 1976-09-08 | Detection device for all carrier single sideband signals |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5333042A JPS5333042A (en) | 1978-03-28 |
| JPS6016761B2 true JPS6016761B2 (en) | 1985-04-27 |
Family
ID=14480236
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP10826476A Expired JPS6016761B2 (en) | 1976-09-08 | 1976-09-08 | Detection device for all carrier single sideband signals |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6016761B2 (en) |
-
1976
- 1976-09-08 JP JP10826476A patent/JPS6016761B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5333042A (en) | 1978-03-28 |
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