JPH0479497B2 - - Google Patents

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Publication number
JPH0479497B2
JPH0479497B2 JP16210987A JP16210987A JPH0479497B2 JP H0479497 B2 JPH0479497 B2 JP H0479497B2 JP 16210987 A JP16210987 A JP 16210987A JP 16210987 A JP16210987 A JP 16210987A JP H0479497 B2 JPH0479497 B2 JP H0479497B2
Authority
JP
Japan
Prior art keywords
circuit
signal
output
averaging
absolute value
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
JP16210987A
Other languages
Japanese (ja)
Other versions
JPS645248A (en
Inventor
Susumu Ootani
Tosha Todoroki
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.)
NEC Corp
Original Assignee
Nippon Electric Co Ltd
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 Nippon Electric Co Ltd filed Critical Nippon Electric Co Ltd
Priority to JP16210987A priority Critical patent/JPS645248A/en
Priority to DE3886107T priority patent/DE3886107T2/en
Priority to EP92201171A priority patent/EP0497433B1/en
Priority to DE3854505T priority patent/DE3854505T2/en
Priority to AU18248/88A priority patent/AU594621B2/en
Priority to EP88305685A priority patent/EP0296822B1/en
Priority to CA000570052A priority patent/CA1332450C/en
Priority to US07/210,653 priority patent/US4835790A/en
Publication of JPS645248A publication Critical patent/JPS645248A/en
Publication of JPH0479497B2 publication Critical patent/JPH0479497B2/ja
Priority to CA000616675A priority patent/CA1333922C/en
Granted legal-status Critical Current

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Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は、デイジタル通信システムの受信側に
おいて搬送波電力対雑音電力比(C/N)を測定
するC/N測定回路に関する。
DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to a C/N measuring circuit that measures carrier power to noise power ratio (C/N) on the receiving side of a digital communication system.

(従来の技術) デイジタル通信システムでは、復調器あるいは
復調器を含む伝送路全体の性能を評価するため、
復調器で復号された符号のビツト誤り率(BER)
に対する性能指数として伝送情報1ビツト当りの
エネルギー対雑音電力密度との比(Eb/N0)を
定義するが、これは次の式(1)で示す如く計算によ
つて求められる。
(Prior art) In digital communication systems, in order to evaluate the performance of a demodulator or the entire transmission path including the demodulator,
Bit error rate (BER) of the code decoded by the demodulator
The ratio of the energy per bit of transmitted information to the noise power density (E b /N 0 ) is defined as a figure of merit for the following equation (1).

Eb/N0=C/N・B/R ……(1) ここで、C/Nは搬送波電力対雑音電力比、B
は復調器の等価雑音帯域幅、Rはデータ伝送速で
ある。
E b /N 0 = C/N・B/R ...(1) Here, C/N is the carrier power to noise power ratio, B
is the equivalent noise bandwidth of the demodulator and R is the data transmission rate.

ところで、式(1)から明らかなように、Eb/N0
を求めるにはC/Nを測定する必要がある。そこ
で、例えば衛星回線におけるEb/N0を決定する
場合の従来のC/N測定方式は、第7図に示す如
く、衛星の中継器に比べて狭帯域の復調器72の
前段にバンドパスフイルタ71を配置し、受信変
調信号が入力される復調器72の入力のIF帯で
C/Nを測定するようにしている。
By the way, as is clear from equation (1), E b /N 0
To find this, it is necessary to measure the C/N. Therefore, for example, in the case of determining E b /N 0 in a satellite line, the conventional C/N measurement method uses a band pass at the front stage of the demodulator 72, which has a narrower band than the satellite repeater, as shown in FIG. A filter 71 is arranged to measure the C/N in the IF band of the input of the demodulator 72 into which the received modulated signal is input.

その測定手順は、まずバンドパスフイルタ71
の帯域の中心に無変調波あるいは変調波を送信し
てバンドパスフイルタ71の出力電力を測定しC
+Nを求める。次に、無変調波あるいは変調波の
送信を止めるか、または送信搬送波周波数をずら
して受信信号がバンドパスフイルタ71の帯域外
となるようにしてバンドパスフイルタ71の出力
電力を測定し、Nを求める。そして、先に求めた
C+NからNを引くとCが求まり、両者からC/
Nが求まる。なお、この場合のBはバンドパスフ
イルタの等価雑音帯域幅である。
The measurement procedure begins with the bandpass filter 71.
The output power of the bandpass filter 71 is measured by transmitting an unmodulated wave or a modulated wave to the center of the band of C.
Find +N. Next, the output power of the bandpass filter 71 is measured by stopping the transmission of the unmodulated wave or the modulated wave, or by shifting the transmission carrier frequency so that the received signal is outside the band of the bandpass filter 71. demand. Then, by subtracting N from the C+N obtained earlier, C is obtained, and from both, C/
Find N. Note that B in this case is the equivalent noise bandwidth of the bandpass filter.

(発明が解決しようとする問題点) しかし、前述した従来のC/N測定方式には次
の如き種々の問題点がある。
(Problems to be Solved by the Invention) However, the conventional C/N measurement method described above has the following various problems.

まず、正確な等価雑音帯域幅が既知であるバン
ドパスフイルタが測定用として必要であり、ま
た、電力計等の測定器が別に必要である。
First, a bandpass filter whose accurate equivalent noise bandwidth is known is required for measurement, and a separate measuring device such as a power meter is also required.

また、C/Nの測定では無変調波あるいは変調
波を送信し、それを止めるか周波数をずらす操作
をIF帯においてするので、操作が繁雑であるだ
けでなく、運用状態においてC/N測定を行うこ
とが困難である。
In addition, in C/N measurement, unmodulated waves or modulated waves are transmitted, and operations to stop or shift the frequency are performed in the IF band, which not only makes the operation complicated, but also requires C/N measurement during operational conditions. Difficult to do.

そこで、この問題に対処し運用時のC/N測定
を可能にする方策として、復調器で生成される受
信基底帯域信号列から信号成分と雑音成分の電力
をそれぞれ推定することが考えられる。
Therefore, as a measure to deal with this problem and enable C/N measurement during operation, it is conceivable to estimate the power of the signal component and the noise component, respectively, from the received baseband signal sequence generated by the demodulator.

即ち、受信信号中の信号成分をS(t)、雑音成
分をN(t)とすると、雑音成分はガウス分布と
みなせるので、その平均()は()=0と
なる。つまり、受信信号について平均化処理を施
せば信号成分S(t)を取り出すことができる。
That is, if the signal component in the received signal is S(t) and the noise component is N(t), the noise component can be regarded as a Gaussian distribution, so the average () is ()=0. That is, by performing averaging processing on the received signal, the signal component S(t) can be extracted.

なお、信号点位置を揃える必要があるので、平
均化処理の前に受信信号について絶対値をとる操
作を行う。故に、平均化処理をしたものについて
2乗処理を施せば信号電力を得ることができる。
即ち、 P={()+()}2 ={()+()}2={()}2 ……(2) 一方、受信信号{S(t)+N(t)}について2
乗処理、平均化処理を行えば、信号は {()+()}2=()2+(
2+2()() =()2+()2+2(
)()……(3) となる。そして、式(3)において()=0の条
件から第3項は消滅するので、次の式(4)となる。
Note that since it is necessary to align the signal point positions, an operation is performed to obtain the absolute value of the received signal before the averaging process. Therefore, the signal power can be obtained by performing squaring processing on the averaged signal.
That is, P={()+()} 2 = {()+()} 2 = {()} 2 ...(2) On the other hand, for the received signal {S(t)+N(t)} 2
After multiplication and averaging, the signal becomes {() + ()} 2 = () 2 + (
) 2 +2()() =() 2 +() 2 +2(
)()……(3). In equation (3), the third term disappears due to the condition ( ) = 0, so the following equation (4) is obtained.

{()+()}2 =()2+()2 ……(4) 斯くして、式(2)と同(4)からC/Nを求めること
ができる。
{()+()} 2 = () 2 + () 2 ... (4) Thus, C/N can be determined from equations (2) and (4).

ところで、受信信号が例えば2値のデイジタル
信号に係るものである場合、ガウス雑音が重畳し
た受信信号振幅値の確率密度分布は第3図aの
イ,ロに示す如くなる。
By the way, when the received signal is related to, for example, a binary digital signal, the probability density distribution of the received signal amplitude value on which Gaussian noise is superimposed is as shown in A and B of FIG. 3A.

即ち、高C/N条件下では受信信号の振幅値の
確率密度分布は信号点位置Sを中心とした曲線イ
のようなガウス分布の示す。この場合には、絶対
値操作によつて信号点位置−Sの受信信号を信号
点位置S側に折り返しても曲線イと同様の確率密
度分布になるので、絶対値操作後における受信信
号系列の平均はほぼ信号点位置Sにおける振幅値
に等しくなる。一方、低C/N条件下では受信信
号に重畳される雑音電力が増加するので、受信信
号の振幅値の確率密度分布は曲線ロに示す如く裾
野が広がり中間位置0を超えて信号点位置−Sの
近傍にまで達するものとなる。
That is, under high C/N conditions, the probability density distribution of the amplitude value of the received signal shows a Gaussian distribution like curve A centered at the signal point position S. In this case, even if the received signal at signal point position -S is returned to the signal point position S side by absolute value manipulation, the probability density distribution will be similar to that of curve A, so the received signal sequence after absolute value manipulation will be The average is approximately equal to the amplitude value at the signal point position S. On the other hand, under low C/N conditions, the noise power superimposed on the received signal increases, so the probability density distribution of the amplitude value of the received signal broadens at the base as shown in curve B and goes beyond the intermediate position 0 to the signal point position - It reaches close to S.

すると、絶対値操作によつて信号点位置−Sの
受信信号を信号点位置S側に折り返した場合、受
信信号の振幅値の確率密度分布は曲線ハに示す如
く信号点位置Sを中心として左右非対称となる。
つまり、受信信号系列の平均は信号点位置Sにお
ける振幅値と異なることになる。その結果、第6
図に示す如く、高C/N条件下では高精度の測定
を行えるが、C/N条件が低下した7dB以下では
次第に理想値から離れて行き、誤差が大きくな
る。
Then, when the received signal at the signal point position -S is returned to the signal point position S side by absolute value manipulation, the probability density distribution of the amplitude value of the received signal will change left and right around the signal point position S as shown in curve C. It becomes asymmetrical.
In other words, the average of the received signal sequence is different from the amplitude value at the signal point position S. As a result, the 6th
As shown in the figure, highly accurate measurements can be made under high C/N conditions, but when the C/N conditions drop below 7 dB, the values gradually deviate from the ideal value and the error increases.

以上要するに、復調器で生成される受信機低帯
域信号列から信号成分と雑音成分の電力をそれぞ
れ推定するようにすれば、測定器や繁雑な操作を
要さずに運用時のC/N測定を可能にする。
In summary, if the power of the signal component and noise component are estimated from the receiver low-band signal sequence generated by the demodulator, C/N measurement during operation can be performed without the need for measuring instruments or complicated operations. enable.

しかし、信号電力の推定には絶対値操作が不可
欠となるので、低C/N条件下では折り返しによ
る影響が大きくなる結果測定精度が悪くなるとい
う問題点がある。
However, since absolute value manipulation is essential for estimating signal power, there is a problem that under low C/N conditions, the influence of aliasing increases, resulting in poor measurement accuracy.

本発明は、このような問題点に鑑みなされたも
ので、その目的は、運用時にC/N測定を行う場
合において、低C/N条件下でも精度良くC/N
測定を行うことができるC/N測定回路を提供す
ることにある。
The present invention was made in view of these problems, and its purpose is to accurately measure C/N even under low C/N conditions when performing C/N measurement during operation.
An object of the present invention is to provide a C/N measurement circuit that can perform measurements.

(問題点を解決するための手段) 前記目的を達成するために、本発明のC/N測
定回路は次の如き構成を有する。即ち、本発明の
C/N測定回路は、デイジタル通信システムの受
信側において搬送波電力対雑音電力比(C/N)
を測定するC/N測定回路であつて;受信基底帯
域信号列を入力としその絶対値をとる絶対値回路
と;前記絶対値回路の出力について予め設定した
所定の重み付けを行う重み付回路と;前記重み付
回路の出力について平均化処理を行う第1の平均
回路と;前記第1の平均回路の出力について2乗
操作を行う第1の2乗回路と;前記受信基底帯域
信号列を入力としその2乗操作を行う第2の2乗
回路と;前記第2の2乗回路の出力について平均
化処理を行う第2の平均回路と;前記第1の2乗
回路と前記第2の平均回路の出力を受けて前記比
(C/N)を計算し出力するC/N計算回路と;
を備えたことを特徴とするものである。
(Means for Solving the Problems) In order to achieve the above object, the C/N measuring circuit of the present invention has the following configuration. That is, the C/N measuring circuit of the present invention measures the carrier power to noise power ratio (C/N) on the receiving side of a digital communication system.
A C/N measurement circuit for measuring the C/N ratio; an absolute value circuit that receives a received baseband signal sequence as input and takes its absolute value; a weighting circuit that performs predetermined weighting on the output of the absolute value circuit; a first averaging circuit that performs an averaging process on the output of the weighting circuit; a first squaring circuit that performs a squaring operation on the output of the first averaging circuit; and a first squaring circuit that receives the received baseband signal sequence as an input. a second squaring circuit that performs the squaring operation; a second averaging circuit that performs averaging processing on the output of the second squaring circuit; the first squaring circuit and the second averaging circuit; a C/N calculation circuit that calculates and outputs the ratio (C/N) upon receiving the output of;
It is characterized by having the following.

(作用) 次に、前記の如く構成される本発明のC/N測
定回路の作用を説明する。
(Operation) Next, the operation of the C/N measurement circuit of the present invention configured as described above will be explained.

受信基底帯域信号列は、まず絶対値回路におい
て絶対値がとられた後、重み付回路において低
C/N条件下で生ずる折り返しの影響が最も大き
い部分の寄与を滅ずべく予め設定した所定の重み
付け処理に付される。ここで、重み付関数には、
例えば次のものが考えられる。xを絶対値回路の
出力信号、THを閾値とすると、 (1) W(x)=x (2) W(x)=1 x>TH =0 x≦TH (3) W(x)=1 x>TH =−α x≦TH (4) W(x)=x2 そして、この重み付回路の出力は第1の平均回
路に入力され、短期変動分(雑音成分)が除去さ
れ信号成分が抽出される。今、S(t)を信号成
分、N(t)を雑音成分、W(u)(但し、u=|
S(t)+N(t)|)を前記重み付関数とすると、
第1の平均回路の出力は |()+()|() となるから、第1の2乗回路の出力は |()+()|()2 ……(5) となる。式(5)において、()=0、()・
W(u)0となるので、 |()+()|()2 ≒()・()2 ……(6) となり、これを信号電力()2とする。
First, the absolute value of the received baseband signal sequence is taken in an absolute value circuit, and then a predetermined value is determined in a weighting circuit in order to eliminate the contribution of the portion where the influence of aliasing that occurs under low C/N conditions is the greatest. Subjected to weighting processing. Here, the weighting function is
For example, the following can be considered. If x is the output signal of the absolute value circuit and TH is the threshold, (1) W(x)=x (2) W(x)=1 x>TH =0 x≦TH (3) W(x)=1 x>TH =-α x≦TH (4) W(x)=x 2The output of this weighting circuit is input to the first averaging circuit, where short-term fluctuations (noise components) are removed and signal components are Extracted. Now, S(t) is the signal component, N(t) is the noise component, and W(u) (where u=|
If S(t)+N(t)|) is the weighting function,
Since the output of the first averaging circuit is |()+()|(), the output of the first square circuit is |()+()|() 2 ...(5). In equation (5), ()=0, ()・
Since W(u)0, |()+()|() 2 ≒()・() 2 ...(6) This is taken as the signal power () 2 .

これがC/N計算回路の一方の入力となる。 This becomes one input of the C/N calculation circuit.

一方、受信基底帯域信号列は第2の2乗回路を
介して第2の平均回路へ入力するので、第2の平
均回路の出力は (()+())2 ……(7) となる。S(t)とN(t)は無相関であり、
(t)=0であることを考慮して式(7)を整理する
と (()2+()2 ……(8) となる。これがC/N計算回路の他方の入力とな
る。
On the other hand, the received baseband signal sequence is input to the second averaging circuit via the second square circuit, so the output of the second averaging circuit is (()+()) 2 ...(7) . S(t) and N(t) are uncorrelated,
When formula (7) is rearranged taking into account that (t)=0, it becomes (() 2 +() 2 . . . (8). This becomes the other input of the C/N calculation circuit.

斯くして、C/N計算回路では、式(6)と同(8)に
基づいてC/Nを計算でき、測定C/Nを出力で
きることになる。
In this way, the C/N calculation circuit can calculate the C/N based on equations (6) and (8), and can output the measured C/N.

以上説明したように、本発明のC/N測定回路
によれば、絶対値操作をした信号に重み付処理を
行い、低C/N条件下で生ずる折り返しの影響を
減じた後に平均化処理を行うようにしたので、低
C/N条件下における信号電力の推定精度を高め
ることができ、低C/N条件下でも精度良くC/
N測定を行うことができる。
As explained above, according to the C/N measurement circuit of the present invention, weighting processing is performed on the signal subjected to absolute value manipulation to reduce the influence of aliasing that occurs under low C/N conditions, and then averaging processing is performed. By doing this, it is possible to improve the accuracy of estimating signal power under low C/N conditions.
N measurements can be made.

(実施例) 以下、本発明の実施例を図面を参照して説明す
る。
(Example) Hereinafter, an example of the present invention will be described with reference to the drawings.

第1図は本発明の一実施例に係るC/N測定回
路を示す。第1図において、101は絶対値回
路、102は重み付回路、103は第1の平均回
路、104は第1の2乗回路、106は第2の平
均回路、107はC/N計算回路である。
FIG. 1 shows a C/N measuring circuit according to an embodiment of the present invention. In FIG. 1, 101 is an absolute value circuit, 102 is a weighting circuit, 103 is a first averaging circuit, 104 is a first square circuit, 106 is a second averaging circuit, and 107 is a C/N calculation circuit. be.

以上の構成において、受信基底帯域信号列は入
力端子1へ印加され、絶対値回路101と第2の
2乗回路105とへそれぞれ供給される。
In the above configuration, the received baseband signal sequence is applied to the input terminal 1 and supplied to the absolute value circuit 101 and the second square circuit 105, respectively.

絶対値回路101は入力信号に絶対値操作を行
い、その出力信号を重み付回路102へ出力す
る。
The absolute value circuit 101 performs absolute value manipulation on the input signal and outputs the output signal to the weighting circuit 102 .

重み付回路102は、例えば第2図に示す如く
構成される。これは前記(3)に示す重み付け関数に
よる重み付処理を実現するものであつて、比較器
201と、乗算器202と、セレクタ203とで
基本的に構成される。比較器201では、絶対値
回路101の出力信号と閾値THのレベル比較を
行い、その結果をセレクタ203へ選択制御信号
として与える。例えば、(出力信号)>(閾値TH)
のとき選択制御信号を“1”レベルに設定し、ま
た逆の場合には“0”レベルに設定する。
The weighting circuit 102 is configured as shown in FIG. 2, for example. This implements weighting processing using the weighting function shown in (3) above, and is basically composed of a comparator 201, a multiplier 202, and a selector 203. The comparator 201 compares the levels of the output signal of the absolute value circuit 101 and the threshold value TH, and provides the result to the selector 203 as a selection control signal. For example, (output signal) > (threshold TH)
In this case, the selection control signal is set to "1" level, and in the opposite case, it is set to "0" level.

一方、乗算器202は絶対値回路101の出力
信号と重み付け定数−αとの演算を行い、それを
セレクタ203の一方の入力へ与える。その結
果、セレクタ203では、他方の入力へ絶対値回
路101の出力信号が直接供給されているので、
選択制御信号が“1”のときは絶対値回路101
の出力信号をそのまま出力し、選択制御信号が
“0”のときは乗算器202の出力を選択出力す
る。
On the other hand, the multiplier 202 performs an operation on the output signal of the absolute value circuit 101 and the weighting constant -α, and supplies the result to one input of the selector 203 . As a result, in the selector 203, the output signal of the absolute value circuit 101 is directly supplied to the other input.
When the selection control signal is “1”, the absolute value circuit 101
The output signal of the multiplier 202 is output as is, and when the selection control signal is "0", the output of the multiplier 202 is selectively output.

要するに、この重み付回路102では、第3図
bに示す如く、受信基底帯域信号列が2値のデイ
ジタル信号に係るものである場合、両信号点位置
の中間位置0から信号点位置Sに向かい適宜距離
進んだ点に閾値THを設定し、低C/N条件下に
おいて分布曲線ハとなるところを分布曲線ニとな
るようにする。このとき、重み付け定数−αは折
り返しによる影響の最も大きい部分の寄与が減じ
られるように適宜に設定してある。なお、第3図
はα=0の場合を示す。
In short, in this weighting circuit 102, when the received baseband signal sequence is related to a binary digital signal, as shown in FIG. A threshold value TH is set at a point where a suitable distance has passed, so that the distribution curve C becomes the distribution curve D under low C/N conditions. At this time, the weighting constant -α is appropriately set so that the contribution of the portion most affected by folding is reduced. Note that FIG. 3 shows the case where α=0.

この重み付回路102の出力は第1の平均回路
103を介して第1の2乗回路104へ入力する
ので、第1の2乗回路104の出力は、前記式(6)
で示され、信号電力()2が得られる。これが
C/N計算回路107の一方の入力となる。
The output of this weighting circuit 102 is input to the first squaring circuit 104 via the first averaging circuit 103, so the output of the first squaring circuit 104 is expressed by the above equation (6).
and the signal power () 2 is obtained. This becomes one input of the C/N calculation circuit 107.

一方、受信基底帯域信号列は第2の2乗回路1
05を介して第2の平均回路106へ入力するの
で、第2の平均回路106の出力には、式(8)で示
される電力が得られ、これがC/N計算回路10
7の他方の入力となる。
On the other hand, the received baseband signal sequence is transmitted to the second square circuit 1.
05 to the second averaging circuit 106, the output of the second averaging circuit 106 obtains the power shown by equation (8), which is then input to the C/N calculation circuit 10.
This is the other input of 7.

C/N計算回路107は、例えば第4図に示す
如く、減算回路401と変換テーブル402とで
基本的に構成され、また同図中、符号404は第
1の2乗回路104の出力、符号403は第2の
平均回路106の出力である。減算回路401で
は、前記式(6)と同(8)から ()2+()2−()・()2 の減算処理が施され、雑音電力()2を内容と
する信号405が変換テーブル402へ与えられ
る。変換テーブル402にはさらに信号404も
入力している。この変換テーブル402はROM
からなり、 10log(信号404)−10log(信号405) が記憶されている。つまり、信号404と同40
5をアドレスとして、比(C/N)を内容とする
信号406が出力端子7へ出力される。
The C/N calculation circuit 107 basically consists of a subtraction circuit 401 and a conversion table 402, as shown in FIG. 403 is the output of the second averaging circuit 106. In the subtraction circuit 401, the subtraction process of () 2 + () 2 - () · () 2 is performed from the above equations (6) and (8), and the signal 405 whose content is the noise power () 2 is converted. is provided to table 402. A signal 404 is also input to the conversion table 402 . This conversion table 402 is ROM
10log (signal 404) - 10log (signal 405) is stored. In other words, the signal 404 and the same 40
5 as the address, a signal 406 containing the ratio (C/N) is output to the output terminal 7.

最後に、第5図は、閾値TH=0.25、重み付け
定数−α=−0.5として得られた特性図である。
Finally, FIG. 5 is a characteristic diagram obtained with threshold value TH=0.25 and weighting constant -α=-0.5.

第6図との比較において明らかなように、低
C/N条件下でも4dBまで近似精度が向上してい
る。
As is clear from the comparison with FIG. 6, the approximation accuracy has improved to 4 dB even under low C/N conditions.

(発明の効果) 以上説明したように、本発明のC/N測定回路
によれば、絶対値操作をした信号に重み付処理を
行い、低C/N条件下で生ずる折り返しの影響を
減じた後に平均化処理を行うようにしたので、低
C/N条件下における信号電力の推定精度を高め
ることができ、低C/N条件下でも精度良くC/
N測定を行うことができる。
(Effects of the Invention) As explained above, according to the C/N measurement circuit of the present invention, weighting processing is performed on the signal subjected to absolute value manipulation to reduce the influence of aliasing that occurs under low C/N conditions. Since averaging processing is performed later, the accuracy of estimating signal power under low C/N conditions can be increased, and even under low C/N conditions, C/N can be accurately calculated.
N measurements can be made.

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

第1図は本発明の一実施例に係るC/N測定回
路の構成ブロツク図、第2図は重み付回路の構成
ブロツク図、第3図はガウス雑音が重畳した場合
の受信信号振幅値の確率密度分布図、第4図は
C/N計算回路の構成ブロツク図、第5図は本発
明の重み付処理を付加した場合の特性比較図、第
6図は絶対値操作、平均化処理によつて信号電力
を推定する場合の特性比較図、第7図は従来の
C/N測定回路の構成ブロツク図である。 71……バンドパスフイルタ、72……復調
器、101……絶対値回路、102……重み付回
路、103……第1の平均回路、104……第1
の2乗回路、105……第2の2乗回路、106
……第2の平均回路、107……C/N計算回
路、201……比較器、202……乗算器、20
3……セレクタ、401……減算回路、402…
…変換テーブル。
Fig. 1 is a block diagram of the configuration of a C/N measuring circuit according to an embodiment of the present invention, Fig. 2 is a block diagram of the weighting circuit, and Fig. 3 shows the received signal amplitude value when Gaussian noise is superimposed. Probability density distribution diagram, Figure 4 is a block diagram of the configuration of the C/N calculation circuit, Figure 5 is a characteristic comparison diagram when weighting processing of the present invention is added, Figure 6 is a diagram of absolute value manipulation and averaging processing. FIG. 7 is a characteristic comparison diagram for estimating signal power. FIG. 7 is a block diagram of a conventional C/N measurement circuit. 71... Band pass filter, 72... Demodulator, 101... Absolute value circuit, 102... Weighting circuit, 103... First averaging circuit, 104... First
square circuit, 105...second square circuit, 106
... Second averaging circuit, 107 ... C/N calculation circuit, 201 ... Comparator, 202 ... Multiplier, 20
3...Selector, 401...Subtraction circuit, 402...
...conversion table.

Claims (1)

【特許請求の範囲】[Claims] 1 デイジタル通信システムの受信側において搬
送波電力対雑音電力比(C/N)を測定するC/
N測定回路であつて;受信基底帯域信号列を入力
としその絶対値をとる絶対値回路と;前記絶対値
回路の出力について予め設定した所定の重み付け
を行う重み付回路と;前記重み付回路の出力につ
いて平均化処理を行う第1の平均回路と;前記第
1の平均回路の出力について2乗操作を行う第1
の2乗回路と;前記受信基底帯域信号列を入力と
しその2乗操作を行う第2の2乗回路と;前記第
2の2乗回路の出力について平均化処理を行う第
2の平均回路と;前記第1の2乗回路と前記第2
の平均回路の出力を受けて前記比(C/N)を計
算し出力するC/N計算回路と;を備えているこ
とを特徴とするC/N測定回路。
1 C/N measuring the carrier power to noise power ratio (C/N) on the receiving side of a digital communication system
N measurement circuit; an absolute value circuit that receives a received baseband signal sequence as input and takes its absolute value; a weighting circuit that performs predetermined weighting on the output of the absolute value circuit; a first averaging circuit that performs an averaging process on the output; a first averaging circuit that performs a squaring operation on the output of the first averaging circuit;
a second squaring circuit that receives the received baseband signal sequence as input and performs a squaring operation; a second averaging circuit that performs averaging processing on the output of the second squaring circuit; ; the first square circuit and the second
A C/N measuring circuit comprising: a C/N calculation circuit that receives an output of an average circuit, calculates and outputs the ratio (C/N);
JP16210987A 1987-06-23 1987-06-29 C/n measuring circuit Granted JPS645248A (en)

Priority Applications (9)

Application Number Priority Date Filing Date Title
JP16210987A JPS645248A (en) 1987-06-29 1987-06-29 C/n measuring circuit
EP88305685A EP0296822B1 (en) 1987-06-23 1988-06-22 Carrier-to-noise detector for digital transmission systems
EP92201171A EP0497433B1 (en) 1987-06-23 1988-06-22 Phase controlled demodulation system for digital communication
DE3854505T DE3854505T2 (en) 1987-06-23 1988-06-22 Phase-controlled demodulation device for digital communication.
AU18248/88A AU594621B2 (en) 1987-06-23 1988-06-22 Carrier-to-noise detector for digital transmission systems
DE3886107T DE3886107T2 (en) 1987-06-23 1988-06-22 Carrier / noise detector for digital transmission systems.
CA000570052A CA1332450C (en) 1987-06-23 1988-06-22 Carrier-to-noise detector for digital transmission systems
US07/210,653 US4835790A (en) 1987-06-23 1988-06-23 Carrier-to-noise detector for digital transmission systems
CA000616675A CA1333922C (en) 1987-06-23 1993-07-22 Phase controlled demodulation system for digital communication

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP16210987A JPS645248A (en) 1987-06-29 1987-06-29 C/n measuring circuit

Publications (2)

Publication Number Publication Date
JPS645248A JPS645248A (en) 1989-01-10
JPH0479497B2 true JPH0479497B2 (en) 1992-12-16

Family

ID=15748213

Family Applications (1)

Application Number Title Priority Date Filing Date
JP16210987A Granted JPS645248A (en) 1987-06-23 1987-06-29 C/n measuring circuit

Country Status (1)

Country Link
JP (1) JPS645248A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP7066233B1 (en) * 2021-05-24 2022-05-13 エレックス工業株式会社 AD converter and wideband noise power measuring device and power spectrum measuring device using this

Also Published As

Publication number Publication date
JPS645248A (en) 1989-01-10

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