JPH03932B2 - - Google Patents

Info

Publication number
JPH03932B2
JPH03932B2 JP10838383A JP10838383A JPH03932B2 JP H03932 B2 JPH03932 B2 JP H03932B2 JP 10838383 A JP10838383 A JP 10838383A JP 10838383 A JP10838383 A JP 10838383A JP H03932 B2 JPH03932 B2 JP H03932B2
Authority
JP
Japan
Prior art keywords
signal
output
circuit
amplitude
cos
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
Application number
JP10838383A
Other languages
Japanese (ja)
Other versions
JPS60122A (en
Inventor
Masanori Jinriki
Michasu Kyosue
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.)
BOEICHO GIJUTSU KENKYU HONBUCHO
Original Assignee
BOEICHO GIJUTSU KENKYU HONBUCHO
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 BOEICHO GIJUTSU KENKYU HONBUCHO filed Critical BOEICHO GIJUTSU KENKYU HONBUCHO
Priority to JP10838383A priority Critical patent/JPS60122A/en
Publication of JPS60122A publication Critical patent/JPS60122A/en
Publication of JPH03932B2 publication Critical patent/JPH03932B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04BTRANSMISSION
    • H04B1/00Details of transmission systems, not covered by a single one of groups H04B3/00 - H04B13/00; Details of transmission systems not characterised by the medium used for transmission
    • H04B1/06Receivers
    • H04B1/10Means associated with receiver for limiting or suppressing noise or interference

Landscapes

  • Engineering & Computer Science (AREA)
  • Computer Networks & Wireless Communication (AREA)
  • Signal Processing (AREA)
  • Radar Systems Or Details Thereof (AREA)
  • Noise Elimination (AREA)

Description

【発明の詳細な説明】 本発明は、互いに近接する無線局が相互に干渉
するとき、相手方の不要な信号を取り除くための
SN比改善回路に関するものである。
[Detailed Description of the Invention] The present invention provides a method for removing unnecessary signals of the other party when wireless stations in close proximity to each other interfere with each other.
This relates to a signal-to-noise ratio improvement circuit.

搬送波に情報をのせて伝送しようとするとき、
その搬送波周波数のまわりにしばしば干渉信号が
存在する。移動式の広帯域レーダにおける相互干
渉、またスプレツト・スペクトラム移動通信方式
における2つの近接した局で生じる相互干渉はス
プレツト・スペクトラムの利用における重要な問
題である。従来、このような干渉波を除去する回
路としては、PLL(Phase−Lock−Loop)を用い
たものや、フイルタによる構成のものがあるが、
比較的帯域の狭い干渉波しか除去できないもので
ある。また線形と非線形の増幅器を組み合せた回
路が提案されているが、入力の雑音振幅がレーレ
分布に近ずくとほとんど干渉波の除去効果がなく
なる欠点のあるものである。
When attempting to transmit information by placing it on a carrier wave,
There are often interfering signals around that carrier frequency. Mutual interference in mobile broadband radars and between two adjacent stations in spread spectrum mobile communication systems is an important problem in the use of spread spectrum. Conventionally, circuits for removing such interference waves include those using PLL (Phase-Lock-Loop) and those configured with filters.
It can only remove interference waves with a relatively narrow band. Also, a circuit that combines linear and nonlinear amplifiers has been proposed, but this circuit has the drawback that it is almost ineffective in removing interference waves when the input noise amplitude approaches the Lehre distribution.

本発明は、線形と非線形の増幅器を効果的に組
合せたものの種であり、上記の欠点を除去し、入
力の雑音振幅分布に無関係に干渉波を有効に除去
抑圧できるSN比改善回路を提供しようとするも
のである。
The present invention is a type of device that effectively combines linear and nonlinear amplifiers, and aims to eliminate the above-mentioned drawbacks and provide an SN ratio improvement circuit that can effectively eliminate and suppress interference waves regardless of the input noise amplitude distribution. That is.

以下、本発明に係るSN比改善回路の実施例を
図面に従つて説明する。
Embodiments of the SN ratio improvement circuit according to the present invention will be described below with reference to the drawings.

第1図において、情報信号S(t)cos{ω0t+θs
(t)}に強い干渉信号I(t)cos{ω0t+θI(t)

が混在した搬送波情報信号Xは、入力端子1を通
して包絡線検波回路2、リミツタ回路4及びほぼ
線形な増幅器7(実質的に線形増幅器として作動
するもの)へ夫々入力される。まずリミツタ回路
4において信号Xは強くリミツトされて信号Cと
なり、このリミツタ回路4で発生した信号Cの高
調波成分は、搬送波の角周波数ω0を中心に持つ
帯域フイルタ5で除去され、振幅がほぼ一定な搬
送波を含む信号Dが取り出される。また包絡線検
波回路2にて包絡線検波された出力Aは、さら
に、低域通過フイルタ3を通過し、この出力Bに
より、振幅変調回路6(または掛算器)で前記信
号Dを振幅変調する。このとき、低域フイルタ3
が干渉波の抑圧に重要な役割を果す。振幅変調出
力Eと、ほぼ線形な増幅器7の出力Fとは差分回
路8に加えられ、両信号の差信号Zが出力端子9
に出力される。
In Fig. 1, the information signal S(t) cos {ω 0 t+θs
(t)} strong interference signal I(t)cos{ω 0 t+θ I (t)
}
The carrier wave information signal X containing a mixture of carrier wave information signals is input through an input terminal 1 to an envelope detection circuit 2, a limiter circuit 4, and a substantially linear amplifier 7 (which operates substantially as a linear amplifier). First, in the limiter circuit 4 , the signal A signal D containing a substantially constant carrier wave is taken out. Further, the output A whose envelope has been detected by the envelope detection circuit 2 further passes through a low-pass filter 3, and the amplitude modulation circuit 6 (or multiplier) modulates the amplitude of the signal D using this output B. . At this time, low-pass filter 3
plays an important role in suppressing interference waves. The amplitude modulated output E and the substantially linear output F of the amplifier 7 are applied to a difference circuit 8, and a difference signal Z between the two signals is sent to an output terminal 9.
is output to.

上記第1図の回路を理論的に考察してみる。第
1図における入力Xは、 X=S(t)cos{ω0t+θs(t)}+I(t) ×cos{ω0t+θI(t)} ……(1) で表わせる。このとき包絡線検波回路出力Aは A=√2()+2()+2()・(
)×{()−I()}……(2) である。いま仮に、干渉信号が情報信号に比べて
相対的に非常に大きい場合を考える。したがつ
て、 S(t)≪I(t) ……(3) が成立つ。このとき(2)式は近的に A≒I(t)+S(t)cos{θs(t)−θI(t)

……(4) と表わせる。ここで干渉信号は第2図示すように
振幅I(t)周波数帯域がS(t)cos{θs(t)−θ
I
(t)}の周波数帯域に比較し、非常に小さい場合
を考える。こような場合は情報信号または干渉信
号が高速な位相変調または周波数変調している場
合に多い。このようなとき、包絡線検波信号Aを
適当な低域フイルタ3に通過させると、(4)式右辺
の第2項の成分をほとんど除去することが出来
る。このとき出力Bは近似的に A≒i(t) ……(5) で表わせる。
Let us theoretically consider the circuit shown in FIG. 1 above. The input X in FIG . 1 can be expressed as : At this time, the envelope detection circuit output A is A=√ 2 () + 2 () + 2 ()・(
) × {() − I ()}……(2). Let us now consider a case where the interference signal is relatively large compared to the information signal. Therefore, S(t)≪I(t)...(3) holds true. In this case, equation (2) is approximately A≒I(t)+S(t) cos {θs(t)−θ I (t)
}
...It can be expressed as (4). Here, as shown in Figure 2, the interference signal has an amplitude I(t) and a frequency band of S(t)cos{θs(t)-θ
I
Consider a case where the frequency band is very small compared to the frequency band of (t)}. Such cases often occur when the information signal or interference signal is subjected to high-speed phase modulation or frequency modulation. In such a case, if the envelope detection signal A is passed through an appropriate low-pass filter 3, most of the component of the second term on the right side of equation (4) can be removed. At this time, output B can be approximately expressed as A≒i(t)...(5).

一方、信号Xがリミツタ回路4で強くリミツト
され、さらに帯域通過フイルタ5で角周波数ω0
の近傍のみを取り出したときの出力Dは、ハード
リミツタ出力の主成分で近似的に表わせ となる。(3)式の条件を考慮すると(6)式は近似的に D≒3/4〔cos{ω0t+θI(t)}+S(t)/2I(
t)×cos{ω0t+θs(t)}−S(t)/2I(t)×
cos{ω0t+2θI(t)−θs(t)}〕
……(7) となる。出力Dは出力Bの信号で振幅変調され
る。したがつて、変調後の出力Eは(5)式に(7)式を
掛けることによつて求まる。
On the other hand, the signal
The output D when extracting only the vicinity of is approximately expressed by the main component of the hard limiter output. becomes. Considering the conditions of equation (3), equation (6) approximately becomes D≒3/4 [cos {ω 0 t+θ I (t)}+S(t)/2I(
t)×cos {ω 0 t+θs(t)}−S(t)/2I(t)×
cos {ω 0 t+2θ I (t)−θs(t)}]
...(7) becomes. Output D is amplitude modulated by the output B signal. Therefore, the output E after modulation can be found by multiplying equation (5) by equation (7).

E≒3/4〔I(t)cos{ω0t+θI(t)}+S(t
)/2×cos{ω0t+θs(t)}−S(t)/2×cos
{ω0t+2θI(t)−θs
(t)}〕 ……(9) 第1図の出力端子9に得られる最終的な出力Z
は、上記出力Eと入力信号Xがほぼ線形な増幅器
を通過した信号Fとの差信号である。このとき、
出来るだけ干渉信号を除去できるようにほぼ線形
な増幅器7の増幅度を調整すると、出力Zは、 Z=3/8〔S(t)cos{ω0t+θs(t)}+S
(t)cos{ω0t+2θI(t)−θs(t)}…(10) となる。ここで、入力Xと出力Zの信号対雑音比
(SIRと略す)を求めてみると、入力のSIR(=
Rin)は Rin=<S2>/<I2> である。ただし、< >平均値を示す。また出力
ZのSIR(=Rout)は(10)式から Rout=<S2>/<S2>=1 となる。したがつて、入力と出力のSIRの改善度
Iは、 I=Rout/Rin=<I2>/<S2> となり、入力のSIRが小さい程非常に大きな改善
が期待できる。
E≒3/4 [I(t)cos{ω 0 t+θ I (t)}+S(t
)/2×cos {ω 0 t+θs(t)}−S(t)/2×cos
0 t+2θ I (t)−θs
(t)}] ...(9) Final output Z obtained at output terminal 9 in Figure 1
is a difference signal between the output E and the signal F obtained by passing the input signal X through a substantially linear amplifier. At this time,
When the amplification degree of the nearly linear amplifier 7 is adjusted so as to remove the interference signal as much as possible, the output Z becomes
(t)cos{ω 0 t+2θ I (t)−θs(t)} (10). Here, when calculating the signal-to-noise ratio (abbreviated as SIR) of input X and output Z, we find that the input SIR (=
Rin) is Rin=<S 2 >/<I 2 >. However, <> indicates the average value. Further, the SIR (=Rout) of the output Z becomes Rout=<S 2 >/<S 2 >=1 from equation (10). Therefore, the degree of improvement I in the input and output SIR is as follows: I=Rout/Rin=<I 2 >/<S 2 >, and the smaller the input SIR, the greater the improvement can be expected.

以上説明したように、本発明のSN比改善回路
によれば、線形と非線形な増幅器を組合せて効果
的な処理を行つているので、近接している無線局
が相互に干渉して生じる、近接局の不要信号を除
去できるものである。
As explained above, according to the signal-to-noise ratio improvement circuit of the present invention, effective processing is performed by combining linear and non-linear amplifiers. It can remove unnecessary signals from the station.

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

第1図は本発明に係るSN比改善回路の実施例
を示すブロツク図、第2図は入力信号の包絡線検
波信号の特徴を示す説明図である。 1……入力端子、2……包絡線検波回路、3…
…低域通過フイルタ、4……リミツタ回路、5…
…帯域通過フイルタ、6……振幅変調器、7……
ほぼ線形な増幅器、8……差分回路。
FIG. 1 is a block diagram showing an embodiment of the SN ratio improving circuit according to the present invention, and FIG. 2 is an explanatory diagram showing the characteristics of an envelope detection signal of an input signal. 1...Input terminal, 2...Envelope detection circuit, 3...
...Low pass filter, 4...Limiter circuit, 5...
...Bandpass filter, 6...Amplitude modulator, 7...
Almost linear amplifier, 8...differential circuit.

Claims (1)

【特許請求の範囲】[Claims] 1 干渉波が混在している搬送波情報信号をリミ
ツタ回路及び高調波除去フイルタに通過させて得
た信号を、前記搬送波情報信号の包絡線検波信号
を低域フイルタに通過させた出力により振幅変調
し、この振幅変調波出力と、前記搬送波情報信号
を線形に近い増幅器で増幅した出力との差信号を
出力することを特徴とするSN比改善回路。
1 A signal obtained by passing a carrier wave information signal containing interference waves through a limiter circuit and a harmonic removal filter is amplitude-modulated by the output of passing an envelope detection signal of the carrier wave information signal through a low-pass filter. , an SN ratio improvement circuit that outputs a difference signal between this amplitude modulated wave output and an output obtained by amplifying the carrier information signal with a nearly linear amplifier.
JP10838383A 1983-06-16 1983-06-16 S/n improving circuit Granted JPS60122A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP10838383A JPS60122A (en) 1983-06-16 1983-06-16 S/n improving circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP10838383A JPS60122A (en) 1983-06-16 1983-06-16 S/n improving circuit

Publications (2)

Publication Number Publication Date
JPS60122A JPS60122A (en) 1985-01-05
JPH03932B2 true JPH03932B2 (en) 1991-01-09

Family

ID=14483374

Family Applications (1)

Application Number Title Priority Date Filing Date
JP10838383A Granted JPS60122A (en) 1983-06-16 1983-06-16 S/n improving circuit

Country Status (1)

Country Link
JP (1) JPS60122A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0761024B2 (en) * 1989-04-10 1995-06-28 防衛庁技術研究本部長 Interference wave remover
US5036154A (en) * 1989-11-15 1991-07-30 The Dow Chemical Company Preparation of glycidyl esters

Also Published As

Publication number Publication date
JPS60122A (en) 1985-01-05

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