JPH0735789A - Device and method for measuring power of spectrum analyzer - Google Patents

Device and method for measuring power of spectrum analyzer

Info

Publication number
JPH0735789A
JPH0735789A JP19918593A JP19918593A JPH0735789A JP H0735789 A JPH0735789 A JP H0735789A JP 19918593 A JP19918593 A JP 19918593A JP 19918593 A JP19918593 A JP 19918593A JP H0735789 A JPH0735789 A JP H0735789A
Authority
JP
Japan
Prior art keywords
power
average
spectrum analyzer
measuring
conversion
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.)
Granted
Application number
JP19918593A
Other languages
Japanese (ja)
Other versions
JP3369651B2 (en
Inventor
Mitsunori Satou
三範 佐藤
Yuji Yoshino
勇治 吉野
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.)
Advantest Corp
Original Assignee
Advantest Corp
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 Advantest Corp filed Critical Advantest Corp
Priority to JP19918593A priority Critical patent/JP3369651B2/en
Publication of JPH0735789A publication Critical patent/JPH0735789A/en
Application granted granted Critical
Publication of JP3369651B2 publication Critical patent/JP3369651B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Abstract

PURPOSE:To provide a device and method for measuring power which can measure a total power and an average power accurately without any error in measuring noise and spectrum diffusion signal. CONSTITUTION:In a spectrum analyzer, an input signal is converted to a genuine number of PPn=10P<n/10> by providing a genuine number conversion part 11. Then, by providing an average value calculation part 12, an average value of PPa=(PP1+PP2+...+PPN) is obtained. Then. by providing a logarithmic conversion part 13, an average power is obtained by Pavg=10logPPa, thus constituting a power measuring instrument. Also, by providing a total power calculation part 14 and by multiplying an average power per unit by a measurement frequency value, a device for obtaining the total power may be configured. Also, the operation may be realized as a method for measuring power.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明はスペクトラムアナライザ
に於いて、一定の手順により平均電力を算出し、又、全
電力を算出する手段を備えた電力測定装置及び方法に関
する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an apparatus and method for measuring power in a spectrum analyzer, which is provided with means for calculating average power by a fixed procedure and calculating total power.

【0002】[0002]

【従来の技術】近年、スペクトル拡散方式の無線システ
ムが提唱されており、これらの無線機の出力パワーの測
定を行う必要がある。スペクトル拡散方式は、信号を通
常の方式よりも広い周波数帯域に拡散し、周波数当たり
の電力を小さくして送信する通信方式である。通常の変
調の他に、さらに拡散符号と呼ばれる高速の符号系列を
用いて、信号の周波数スペクトルを広帯域に拡散するた
めの変調を行う。スペクトル拡散通信方式では、周波数
帯域を広く使用することになるが、信号のエネルギーは
一定であるので、周波数当たりの電力が低くなる。
2. Description of the Related Art In recent years, spread spectrum wireless systems have been proposed, and it is necessary to measure the output power of these wireless devices. The spread spectrum method is a communication method in which a signal is spread over a wider frequency band than a normal method and power per frequency is reduced to be transmitted. In addition to ordinary modulation, a high-speed code sequence called a spreading code is used to perform modulation for spreading the frequency spectrum of the signal in a wide band. In the spread spectrum communication system, the frequency band is widely used, but since the signal energy is constant, the power per frequency is low.

【0003】これまでに、電力の測定を行う場合、電力
計(パワーメータ)やスペクトラムアナライザ等が使用
されている。しかし、パワーメータのセンサーでは、周
波数帯域を任意に設定するのは困難であり、又、電力の
測定幅(ダイナミックレンジ)が+10dBmー−60
dBm程度で狭いという問題点を有する。
Hitherto, when measuring power, a power meter, a spectrum analyzer, etc. have been used. However, with a power meter sensor, it is difficult to arbitrarily set the frequency band, and the power measurement width (dynamic range) is +10 dBm-60.
There is a problem that it is narrow at about dBm.

【0004】そこで、スペクトラムアナライザを用いて
電力測定する場合は、次に述べる方法がとられている。
Therefore, in the case of measuring the power using a spectrum analyzer, the following method is adopted.

【0005】図2は従来のスペクトラムアナライザの構
成を示すブロック図である。
FIG. 2 is a block diagram showing the structure of a conventional spectrum analyzer.

【0006】入力信号は掃引信号発生器7により制御さ
れた電圧制御型局部発振器7の出力とミキサ1を通じて
一定の中間周波数に変更され分解能帯域幅フィルタ2に
入力される。分解能帯域幅フィルタに、たとえばガウシ
アン形のフィルタを採用している場合の帯域幅(ピーク
から3dB下がった点の周波数幅)は、実際の帯域幅に
対して1/2になっている。
The input signal is changed to a constant intermediate frequency through the output of the voltage-controlled local oscillator 7 controlled by the sweep signal generator 7 and the mixer 1 and input to the resolution bandwidth filter 2. When a Gaussian filter, for example, is used as the resolution bandwidth filter, the bandwidth (frequency width at the point where 3 dB falls from the peak) is 1/2 of the actual bandwidth.

【0007】又、分解能帯域幅フィルタは複数段の帯域
幅切替え機能が付いていてスペクトラムアナライイザ最
大の特徴である周波数分析を可能にしている。
Further, the resolution bandwidth filter has a plurality of stages of bandwidth switching functions, and enables the frequency analysis, which is the greatest feature of the spectrum analyzer.

【0008】さらに、信号は分解能帯域フィルタ2か
ら、レベルのダイナミックレンジを広げるための対数増
幅器3に入力され、レベル対周波数に変換され、検波器
4の出力がA/D変換器5でアナログ・ディジタル変換
される。結果は掃引信号発生器の信号で制御された表示
器6により、CRT上に表示される。
Further, the signal is inputted from the resolution band filter 2 to the logarithmic amplifier 3 for expanding the dynamic range of the level, converted into the level versus the frequency, and the output of the detector 4 is converted into an analog signal by the A / D converter 5. Digitally converted. The result is displayed on the CRT by the display 6 controlled by the signal of the sweep signal generator.

【0009】一般に、スペクトラムアナライザの検波法
(スロープ検波法)は、1つのサイン波に対して平均値
検波を行い、一定の換算をして表示が実効値の値に合う
ように構成されている。このため、スペクトラムの広が
りを持った入力信号の場合は、実際の実効値と差異を生
じてしまう。
In general, the detection method (slope detection method) of a spectrum analyzer is configured so that an average value detection is performed on one sine wave and a fixed conversion is performed so that the display matches the value of the effective value. . Therefore, in the case of an input signal having a spread spectrum, there is a difference from the actual effective value.

【0010】又、一般に対数増幅器を通して、スペクト
ラムの広がりを持った信号を平均値検波すると誤差が生
じることが知られている。例えば表示に対する補正はロ
グ・モードで1.05dBに達することが知られてい
る。
Further, it is generally known that an error occurs when a signal having a spectrum spread is detected as an average value through a logarithmic amplifier. For example, the correction for the display is known to reach 1.05 dB in log mode.

【0011】一般に、ランダム雑音のスペクトラム成分
における位相はランダムであり、アナライザの測定帯域
幅を2倍にした場合、測定電圧は2倍にはならず、測定
電力が2倍となる。従って、ランダム雑音は単位帯域幅
あたりの雑音電力(dB/HzあるいはWatt/H
z)で規定されるのが普通である。
Generally, the phase of the spectrum component of random noise is random, and when the measurement bandwidth of the analyzer is doubled, the measurement voltage does not double, but the measurement power doubles. Therefore, the random noise is the noise power per unit bandwidth (dB / Hz or Watt / H
It is usually specified in z).

【0012】又、入力信号がランダム雑音信号の場合に
は、上述のスペクトラムアナライザは分解能帯域幅フィ
ルタを通った雑音を扱うことになり、雑音がレーリー分
布していると仮定すると、これらの差異は対数増幅器で
の圧縮による誤差−2.5dBであると算出できること
が知られている。ここで、レーリ分布とは、散乱の分布
状態を示し、ホワイト雑音の包絡線成分を意味してい
る。
Further, when the input signal is a random noise signal, the above spectrum analyzer handles the noise that has passed through the resolution bandwidth filter, and assuming that the noise is Rayleigh distributed, these differences are It is known that the error due to compression in the logarithmic amplifier can be calculated to be −2.5 dB. Here, the Rayleigh distribution indicates a distribution state of scattering and means an envelope component of white noise.

【0013】[0013]

【発明が解決しようとする課題】以上のように、スペク
トラム拡散信号及びランダム雑音の電力測定を行おうと
する場合、測定しようとする電波の全周波数帯域の測定
が必要であるが、通常の電力計に於いては、測定器のパ
ワーセンサの測定可能帯域幅が全帯域を一つでカバーで
きない為、真の値が得られないという問題点があるので
全帯域をカバーできるスペクトラムアナライザを用いる
のが有利である。
As described above, when attempting to measure the power of a spread spectrum signal and random noise, it is necessary to measure the entire frequency band of the radio wave to be measured. In this case, since the measurable bandwidth of the power sensor of the measuring instrument cannot cover the entire bandwidth by one, there is a problem that a true value cannot be obtained. Therefore, it is recommended to use a spectrum analyzer that can cover the entire bandwidth. It is advantageous.

【0014】しかし、スペクトラム拡散信号及びランダ
ム雑音の電力測定を行おうとする場合、スペクトルが広
帯域に拡散するため、上述の検波方法や、対数増幅方法
では誤差が増大するという問題点を有する。
However, when attempting to measure the power of the spread spectrum signal and the random noise, the spectrum spreads over a wide band, so that the above-mentioned detection method and logarithmic amplification method have a problem that the error increases.

【0015】本発明は、上述したような従来の技術が有
する問題点に鑑みてなされるものであって、雑音やスペ
クトラム拡散信号の電力を測定する場合に、誤差を生ぜ
ず、高精度に全電力測定や平均電力を測定できる電力測
定装置及び方法を提供することを目的とする。
The present invention has been made in view of the problems of the above-mentioned conventional techniques, and when measuring the power of noise or spread spectrum signals, no error is produced and the accuracy is high. An object of the present invention is to provide a power measuring device and method capable of measuring power and measuring average power.

【0016】[0016]

【課題を解決するための手段】この発明によれば、スペ
クトラムアナライザに於て、入力信号をアナログディジ
タル変換した信号を真数変換するための、真数変換部1
1を設ける。これは、入力信号の瞬時値を得るために、
A/D変換器5の出力を電力真数変換するためである。
また、A/D変換器5の出力については、分解能帯域幅
より十分広い帯域幅を持つビデオ帯域幅により増幅する
と(図示はしていない)、スペクトラムアナライザのC
RT表示は信号の瞬時値を表示する。
According to the present invention, in a spectrum analyzer, an antilogarithm converter 1 for performing antilogarithmic conversion of a signal obtained by analog-digital converting an input signal.
1 is set. This is to get the instantaneous value of the input signal,
This is because the output of the A / D converter 5 is converted to the power antilogarithm.
In addition, the output of the A / D converter 5 is amplified by a video bandwidth having a bandwidth sufficiently wider than the resolution bandwidth (not shown).
The RT display shows the instantaneous value of the signal.

【0017】この真数変換部11により、たとえばサン
プル点Xnでの測定レベルPn(dBm)とすると PPn=10Pn/10 (mW) となるように真数変換する。次に、平均値を算出するた
めの平均値算出部12を設ける。そして当該PPnの値
をnが1からNまでのポイントで総和を求め、Nで除し
て、 PPa=(PP1+PP2+・・・+PPN)/N (m
W) となる平均値を得る。次に対数変換するための対数変換
部13を設ける。そして当該PPaの値を対数変換して
avg=10logPPa (mW) により平均電力を得る。このようにPavg(mW)を求
める電力測定装置を構成する。
The antilogarithm conversion unit 11 performs the antilogarithmic conversion so that PP n = 10 Pn / 10 (mW), for example, when the measurement level P n (dBm) at the sample point X n is set. Next, the average value calculation unit 12 for calculating the average value is provided. Then, the sum of the values of PP n is calculated at a point where n is from 1 to N, and is divided by N to obtain PP a = (PP 1 + PP 2 + ... + PP N ) / N (m
W) is obtained. Next, a logarithmic conversion unit 13 for performing logarithmic conversion is provided. Then, the value of PP a is logarithmically converted to obtain the average power by P avg = 10 logPP a (mW). In this way, the power measuring device for obtaining P avg (mW) is configured.

【0018】又、上記の装置に於いて、全電力を算出す
るための、全電力算出部14を設け、分解能帯域幅1H
zに換算した平均電力(mW/Hz)に測定周波数幅
(SPAN)を乗ずることにより、スペクトラムアナラ
イザのCRT上にに表示している全電力を得る手段を追
加して電力測定装置を構成してもよい。
Further, in the above apparatus, a total power calculation unit 14 for calculating the total power is provided, and the resolution bandwidth is 1H.
A power measuring device is configured by adding means for obtaining the total power displayed on the CRT of the spectrum analyzer by multiplying the average power (mW / Hz) converted to z by the measurement frequency width (SPAN). Good.

【0019】又、上記の構成はハードウェア装置を構成
して実現しているが、ソフトウェアの演算方法として式
Further, although the above-mentioned configuration is realized by configuring a hardware device, it is expressed as a software calculation method.

【数1】を満たすような演算、すなわち、入力信号をア
ナログディジタル変換した信号について、サンプル点X
nでの測定レベルPn(dBm)の真数変換を演算し、次
に、平均値を演算し、次に、対数変換して平均電力を演
算し、上記の演算を行うことにより、平均電力を得るよ
うにして電力測定方法として実現してもよい。
For a calculation that satisfies the following equation, that is, for a signal obtained by analog-digital converting the input signal, the sampling point X
calculates the measured level P n antilogarithm conversion (dBm) at n, then calculates the average value, then log-transformed to calculate the average power, by performing the calculation of the average power May be realized as a power measuring method.

【0020】[0020]

【作用】この発明によれば、スペクトラムアナライザに
於て、真数変換部を設け、平均値算出部を設け、対数変
換部を設けたから、一連の演算結果により平均電力を得
ることが可能となる。
According to the present invention, in the spectrum analyzer, the antilogarithm conversion unit, the average value calculation unit, and the logarithm conversion unit are provided, so that the average power can be obtained by a series of calculation results. .

【0021】さらに、上記の装置に、全電力算出部を追
加して設けて、スペクトラムアナライザに表示している
全電力を得ることも可能となる。
Furthermore, it is possible to obtain the total power displayed on the spectrum analyzer by additionally providing the above-mentioned device with a total power calculation section.

【0022】又、上記の構成はハードウェア装置を構成
して実現しているが、ソフトウェアの演算方法として式
Further, although the above-mentioned configuration is realized by configuring a hardware device, it is expressed as a software calculation method.

【数1】を満たすような一連の演算を行うことにより平
均電力や全電力を得ることも可能となる。
It is also possible to obtain the average power and the total power by performing a series of calculations that satisfy the following equation.

【0023】[0023]

【実施例】本発明の実施例について図面を参照して説明
する。
Embodiments of the present invention will be described with reference to the drawings.

【0024】図1は本発明の構成を示すブロック図であ
る。
FIG. 1 is a block diagram showing the configuration of the present invention.

【0025】図3は本発明の演算を示す概念図である。FIG. 3 is a conceptual diagram showing the operation of the present invention.

【0026】入力信号はA/D変換器5を通って、アナ
ログディジタル変換され、真数変換部11に与えられ
る。
The input signal passes through the A / D converter 5 and undergoes analog-to-digital conversion and is given to the antilogarithm conversion unit 11.

【0027】スペクトラムアナライザに於てはサンプル
点Xnでの測定レベルPnが測定できる。
The spectrum analyzer can measure the measurement level P n at the sample point X n .

【0028】真数変換部11に於いては、この測定レベ
ルPn(dBm)を PPn=10Pn/10 (mW) となるように真数変換する。
In the antilogarithm conversion unit 11, the antilogarithmic conversion of the measurement level P n (dBm) is carried out so that PP n = 10 Pn / 10 (mW).

【0029】次に平均値算出部12に於いては、PPn
の値をnが1からNまでのポイントで総和を求め、Nで
除して、 PPa=(PP1+PP2+・・・+PPN)/N (m
W) となる平均値を得る。
Next, in the average value calculation unit 12, PP n
Value is calculated at a point where n is from 1 to N, divided by N, and PP a = (PP 1 + PP 2 + ... + PP N ) / N (m
W) is obtained.

【0030】次に、対数変換部13に於いては、PPa
の値を対数変換して、 Pavg=10logPPa (mW) により平均電力を得る。
Next, in the logarithmic converter 13, PP a
The value of is logarithmically converted, and the average power is obtained by P avg = 10 logPP a (mW).

【0031】又、平均電力(mW)をスペクトラムアナ
ライザの測定雑音電力帯域幅(Bn)で除することによ
り1Hz当たりの平均電力P(mW/Hz)を求めるこ
とができる。
The average power P (mW / Hz) per 1 Hz can be obtained by dividing the average power (mW) by the measured noise power bandwidth (Bn) of the spectrum analyzer.

【0032】さらに、全電力算出部14に於いて、1H
z当たりの平均電力(mW/Hz)に測定周波数幅(S
PAN)を乗ずることにより、スペクトラムアナライザ
に表示している全電力を得ることができる。
Further, in the total power calculation unit 14, 1H
Average frequency per z (mW / Hz) and measured frequency width (S
By multiplying it by PAN), the total power displayed on the spectrum analyzer can be obtained.

【0033】[0033]

【発明の効果】以上説明したように本考案は構成されて
いるので、次に記載する効果を奏する。
Since the present invention is constructed as described above, it has the following effects.

【0034】雑音やスペクトラム拡散信号の電力を測定
する場合に、誤差を生ぜず、高精度に全電力測定や平均
電力を測定できる。
When measuring the power of noise and spread spectrum signals, the total power and average power can be measured with high accuracy without causing an error.

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

【図1】本発明の構成を示すブロック図である。FIG. 1 is a block diagram showing a configuration of the present invention.

【図2】従来のスペクトラムアナライザの構成を示すブ
ロック図である。
FIG. 2 is a block diagram showing a configuration of a conventional spectrum analyzer.

【図3】本発明の演算を示す概念図である。FIG. 3 is a conceptual diagram showing an operation of the present invention.

【符号の説明】[Explanation of symbols]

1 ミキサ 2 分解能帯域幅フィルタ 3 対数増幅器 4 検波器 5 A/D変換器 6 表示器 7 掃引信号発生器 11 真数変換部 12 平均値算出部 13 対数変換部 14 全電力算出部 1 mixer 2 resolution bandwidth filter 3 logarithmic amplifier 4 detector 5 A / D converter 6 display 7 sweep signal generator 11 antilogarithm converter 12 average value calculator 13 logarithmic converter 14 total power calculator

Claims (4)

【特許請求の範囲】[Claims] 【請求項1】 スペクトラムアナライザに於て、 入力信号をアナログディジタル変換した信号を真数変換
するための、真数変換部(11)を設け、サンプル点X
nでの測定レベルPn(dBm)を PPn=10Pn/10 (mW) となるように真数変換し、 その真数出力を平均値算出するための平均値算出部(1
2)を設け、当該PPnの値をnが1からNまでのポイ
ントで総和を求め、Nで除して、 PPa=(PP1+PP2+・・・+PPN)/N (m
W) となる平均値を得、 その平均値出力を対数変換するための対数変換部(1
3)を設け、当該PPaの値を対数変換して Pavg=10logPPa (mW) となる平均電力を得、 上記の各演算部を具備して構成したことを特徴とする電
力測定装置。
1. In a spectrum analyzer, an antilogarithm conversion unit (11) for performing antilogarithmic conversion of a signal obtained by analog-digital conversion of an input signal is provided, and a sampling point X is provided.
measuring levels P n at n the (dBm) and antilogarithm converter such that PP n = 10 Pn / 10 ( mW), the average value calculating unit for averaging the true number of output (1
2) is provided, the value of PP n is summed at the point where n is from 1 to N, and is divided by N to obtain PP a = (PP 1 + PP 2 + ... + PP N ) / N (m
W) to obtain an average value and logarithmically convert the average value output (1)
3) is provided, the value of PP a is logarithmically converted to obtain an average power of P avg = 10 logPP a (mW), and the above-mentioned arithmetic units are provided to configure the power measuring apparatus.
【請求項2】 請求項1記載の装置に於いて、 全電力を算出するための、全電力算出部(14)を設
け、請求項1で得た平均電力 Pavg=10logPPa (mW) を測定雑音電力帯域幅で除した1Hz当たりの平均電力
(mW/Hz)に測定周波数幅(SPAN)を乗ずるこ
とにより、スペクトラムアナライザに表示している全電
力を得、 上記の演算部を具備して構成したことを特徴とする電力
測定装置。
2. The device according to claim 1, further comprising a total power calculation unit (14) for calculating total power, and calculating the average power P avg = 10 logPP a (mW) obtained in claim 1. By multiplying the average power per 1 Hz (mW / Hz) divided by the measurement noise power bandwidth by the measurement frequency width (SPAN), the total power displayed on the spectrum analyzer is obtained, and the above calculation unit is provided. A power measuring device characterized by being configured.
【請求項3】 スペクトラムアナライザで入力信号を測
定する場合に於て、 式 【数1】 を満たすような演算、すなわち、入力信号をアナログデ
ィジタル変換した信号について、サンプル点Xnでの測
定レベルPn(dBm)の真数変換を演算し、次に、平
均値を演算し、次に、対数変換して平均電力を演算し、 上記の演算を行うことにより、平均電力を得ることを特
徴とした電力測定方法。
3. When measuring an input signal with a spectrum analyzer, the following equation is used. That is, for the signal obtained by analog-digital conversion of the input signal, the arithmetic conversion of the measurement level P n (dBm) at the sample point X n is calculated, then the average value is calculated, and then the average value is calculated. A power measuring method characterized by obtaining the average power by performing logarithmic conversion to calculate the average power and performing the above calculation.
【請求項4】 請求項3記載の方法に於いて、 さらに、請求項3で求めた平均電力を測定雑音電力帯域
幅で除した1Hz当たりの平均電力(mW/Hz)に測
定周波数幅(SPAN)を乗ずることにより、スペクト
ラムアナライザに表示している全電力を演算し、 上記の演算を行うことにより、全電力を得ることを特徴
とした電力測定方法。
4. The method according to claim 3, further comprising: an average power per 1 Hz (mW / Hz) obtained by dividing the average power obtained in claim 3 by a measurement noise power bandwidth (SPAN). ) Is calculated to calculate the total power displayed on the spectrum analyzer, and the total power is obtained by performing the above calculation.
JP19918593A 1993-07-16 1993-07-16 Apparatus and method for measuring power of spectrum analyzer Expired - Fee Related JP3369651B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP19918593A JP3369651B2 (en) 1993-07-16 1993-07-16 Apparatus and method for measuring power of spectrum analyzer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP19918593A JP3369651B2 (en) 1993-07-16 1993-07-16 Apparatus and method for measuring power of spectrum analyzer

Publications (2)

Publication Number Publication Date
JPH0735789A true JPH0735789A (en) 1995-02-07
JP3369651B2 JP3369651B2 (en) 2003-01-20

Family

ID=16403556

Family Applications (1)

Application Number Title Priority Date Filing Date
JP19918593A Expired - Fee Related JP3369651B2 (en) 1993-07-16 1993-07-16 Apparatus and method for measuring power of spectrum analyzer

Country Status (1)

Country Link
JP (1) JP3369651B2 (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2003038453A1 (en) * 2001-10-30 2003-05-08 Pearl Kogyo Co., Ltd. High-frequency detection method and high-frequency detection circuit
JP2005084007A (en) * 2003-09-11 2005-03-31 Fujitsu Ltd Band distribution inspection device and band distribution inspection method
CN111030713A (en) * 2019-10-30 2020-04-17 创达特(苏州)科技有限责任公司 Transient pulse interference resisting device and method

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2003038453A1 (en) * 2001-10-30 2003-05-08 Pearl Kogyo Co., Ltd. High-frequency detection method and high-frequency detection circuit
US6958630B2 (en) 2001-10-30 2005-10-25 Pearl Kogyo Co., Ltd. High-frequency detection method and high-frequency detection circuit
CN1300594C (en) * 2001-10-30 2007-02-14 巴尔工业株式会社 High frequency detection method and high frequency detection circuit
JP2005084007A (en) * 2003-09-11 2005-03-31 Fujitsu Ltd Band distribution inspection device and band distribution inspection method
JP4698136B2 (en) * 2003-09-11 2011-06-08 富士通セミコンダクター株式会社 Band distribution inspection device and band distribution inspection method
CN111030713A (en) * 2019-10-30 2020-04-17 创达特(苏州)科技有限责任公司 Transient pulse interference resisting device and method

Also Published As

Publication number Publication date
JP3369651B2 (en) 2003-01-20

Similar Documents

Publication Publication Date Title
US7096133B1 (en) Method of establishing benchmark for figure of merit indicative of amplifier flicker noise
US5808463A (en) Method and apparatus for measuring adjacent channel power using complex fourier transform
US6359429B1 (en) Measuring method using a spectrum analyzer
US8842771B2 (en) Amplitude flatness and phase linearity calibration for RF sources
Jenq Measuring harmonic distortion and noise floor of an A/D converter using spectral averaging
EP0141255B1 (en) Method for measurement by digital spectrum analyzer
JPH058388B2 (en)
CN109164300B (en) Microwave frequency high-precision measurement system and method based on harmonic amplification
CN104076202B (en) signal analysis device and signal analysis method
US20060206550A1 (en) Signal measuring/analyzing apparatus and signal measuring/analyzing method
US6484124B1 (en) System for measurement of selected performance characteristics of microwave components
JP3369651B2 (en) Apparatus and method for measuring power of spectrum analyzer
US20040116080A1 (en) Time resolved RF plasma impedance meter
US20030098682A1 (en) Method and apparatus for spectrum analysis with variable detection latency and multiple layer coherent integrations
EP1305643A1 (en) Signal measurement
US6292000B1 (en) Process for harmonic measurement with enhanced phase accuracy
RU2341808C1 (en) Device for measurement of signal/noise ratio
US6344735B1 (en) Spectrum analyzer and spectrum measuring method using the same
JP3163497B2 (en) Signal analyzer
KR100540248B1 (en) Method for measuring gps air sensitivity and mobile terminal having function of measuring gps air sensitivity
JP2000352569A (en) Spectrum analyzer and its measurement method
KR100417114B1 (en) Apparatus and method to measure high frequency power
JP3416330B2 (en) Adjacent channel leakage power measurement device for wireless devices
JP2004045403A (en) Method and system for measuring noise level of electronic object to be measured
JP2001168836A (en) Transmission power measurement system and method for w-cdma communication system

Legal Events

Date Code Title Description
A02 Decision of refusal

Free format text: JAPANESE INTERMEDIATE CODE: A02

Effective date: 20020423

A01 Written decision to grant a patent or to grant a registration (utility model)

Free format text: JAPANESE INTERMEDIATE CODE: A01

Effective date: 20021015

R250 Receipt of annual fees

Free format text: JAPANESE INTERMEDIATE CODE: R250

R250 Receipt of annual fees

Free format text: JAPANESE INTERMEDIATE CODE: R250

FPAY Renewal fee payment (event date is renewal date of database)

Free format text: PAYMENT UNTIL: 20071115

Year of fee payment: 5

FPAY Renewal fee payment (event date is renewal date of database)

Free format text: PAYMENT UNTIL: 20081115

Year of fee payment: 6

LAPS Cancellation because of no payment of annual fees