JPH0628753U - Jitter measuring device - Google Patents

Jitter measuring device

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Publication number
JPH0628753U
JPH0628753U JP7140292U JP7140292U JPH0628753U JP H0628753 U JPH0628753 U JP H0628753U JP 7140292 U JP7140292 U JP 7140292U JP 7140292 U JP7140292 U JP 7140292U JP H0628753 U JPH0628753 U JP H0628753U
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JP
Japan
Prior art keywords
jitter
signal
under measurement
amount
measuring
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.)
Pending
Application number
JP7140292U
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Japanese (ja)
Inventor
孝文 上原
修治 砂野
Original Assignee
安藤電気株式会社
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 安藤電気株式会社 filed Critical 安藤電気株式会社
Priority to JP7140292U priority Critical patent/JPH0628753U/en
Publication of JPH0628753U publication Critical patent/JPH0628753U/en
Pending legal-status Critical Current

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Abstract

(57)【要約】 【目的】 ジッタを含んだ信号の測定に関して、PLL
構成の位相比較器の非直線性やループ特性の影響を受け
ることなく、単純化した構成で容易な測定を実現するこ
と。 【構成】 ジッタ測定装置15は、基準信号21と被測
定信号23を入力してこの被測定信号23のジッタ量を
測定する装置であり、分周器11とオシロスコープ12
により構成されている。分周器11は、被測定信号23
を入力し、この信号を測定レンジに応じて1/N(Nは
自然数)に分周する分周器である。オシロスコープ12
は、分周信号24と基準信号21を入力し、この基準信
号21をトリガ入力とすることにより、分周信号24に
含まれるジッタ量を測定する測定器である。本実施例で
は、被測定信号23が分周器11で1/N分周されるこ
とで、N/2周期分より小さいジッタ量がオシロスコー
プ12で測定できる。
(57) [Abstract] [Purpose] For measuring signals including jitter, PLL
To realize easy measurement with a simplified structure without being affected by the nonlinearity and loop characteristics of the phase comparator of the structure. [Structure] The jitter measuring device 15 is a device for inputting a reference signal 21 and a signal under measurement 23 to measure the amount of jitter of the signal under measurement 23, and includes a frequency divider 11 and an oscilloscope 12.
It is composed by. The frequency divider 11 has a signal under measurement 23.
Is a frequency divider that divides this signal into 1 / N (N is a natural number) according to the measurement range. Oscilloscope 12
Is a measuring instrument for measuring the amount of jitter contained in the frequency-divided signal 24 by inputting the frequency-divided signal 24 and the reference signal 21 and using the reference signal 21 as a trigger input. In this embodiment, the measured signal 23 is divided by the frequency divider 11 by 1 / N, so that the oscilloscope 12 can measure a jitter amount smaller than N / 2 cycles.

Description

【考案の詳細な説明】[Detailed description of the device]

【0001】[0001]

【産業上の利用分野】[Industrial applications]

本考案はジッタを含んだ被測定信号のジッタ量を測定するジッタ測定装置に関 する。 The present invention relates to a jitter measuring device that measures the amount of jitter of a signal under measurement that includes jitter.

【0002】[0002]

【従来の技術】[Prior art]

従来、ジッタ発生回路で生成された信号のジッタ量を測定する場合、PLL方 式を用いたジッタ測定回路が用いられていた。従来技術によるジッタ測定系の構 成を示す機能ブロック図を図2に示す。 Conventionally, when measuring the amount of jitter of a signal generated by a jitter generating circuit, a jitter measuring circuit using a PLL method has been used. FIG. 2 is a functional block diagram showing the configuration of the jitter measurement system according to the conventional technique.

【0003】 ジッタ発生回路5は、基準信号21とジッタ信号22を入力し、ジッタを含む 被測定信号23を生成する信号発生回路であり、位相比較器1、加算器2、ルー プフィルタ3および電圧制御発振器4で構成される。また、ジッタ測定回路11 は、被測定信号23のジッタ量をPLL方式により測定する測定回路であり、分 周器6・10、位相比較器7、ループフィルタ8および電圧制御発振器9により 構成されている。The jitter generation circuit 5 is a signal generation circuit that inputs a reference signal 21 and a jitter signal 22 and generates a signal under measurement 23 including jitter, and includes a phase comparator 1, an adder 2, a loop filter 3 and a voltage. It is composed of a controlled oscillator 4. The jitter measuring circuit 11 is a measuring circuit for measuring the amount of jitter of the signal under measurement 23 by the PLL method, and is composed of the frequency dividers 6 and 10, the phase comparator 7, the loop filter 8 and the voltage controlled oscillator 9. There is.

【0004】 ジッタ発生回路5は、基準信号21とジッタ信号22を入力し、ジッタ信号2 2のレベルに比例したジッタ量を持つ被測定信号23を生成する。ジッタ発生回 路5により生成された被測定信号23は、ジッタ測定回路11に送られ、測定レ ンジに応じて分周器6により分周され、位相比較器7に送られる。The jitter generating circuit 5 receives the reference signal 21 and the jitter signal 22 and generates a signal under measurement 23 having a jitter amount proportional to the level of the jitter signal 22. The signal under measurement 23 generated by the jitter generating circuit 5 is sent to the jitter measuring circuit 11, is frequency-divided by the frequency divider 6 according to the measurement range, and is sent to the phase comparator 7.

【0005】 位相比較器7はまた、基準信号25を入力し、これら2つの信号を比較し、そ の位相差よりジッタ量を測定する。そして、測定されたジッタ量が出力信号26 としてジッタ測定回路11より出力される。なお、基準信号25は、出力信号2 6を入力するループフィルタ8と、ループフィルタ8からの信号を入力する電圧 制御発振器9、および電圧制御発振器9からの出力を入力する分周器10により 生成される。The phase comparator 7 also receives the reference signal 25, compares these two signals, and measures the amount of jitter from the phase difference. Then, the measured jitter amount is output from the jitter measuring circuit 11 as an output signal 26. The reference signal 25 is generated by the loop filter 8 that inputs the output signal 26, the voltage controlled oscillator 9 that inputs the signal from the loop filter 8, and the frequency divider 10 that inputs the output from the voltage controlled oscillator 9. To be done.

【0006】[0006]

【考案が解決しようとする課題】[Problems to be solved by the device]

図2に示すような従来技術では、ジッタ測定回路11にPLL方式を用いてい るため、ジッタ発生回路5における位相比較器7、ループフィルタ3、電圧制御 発振器4の他に、ジッタ測定回路11において第2の位相比較器7、第2のルー プフィルタ8、第2の電圧制御発振器9が必要になり、構成要素数が増えるとと もに回路構成が複雑になるという欠点がある。さらに従来技術では、位相比較器 7の非直線性の影響やPLLのループ特性の影響を受けるという問題がある。 In the prior art as shown in FIG. 2, since the PLL method is used for the jitter measuring circuit 11, in addition to the phase comparator 7, the loop filter 3 and the voltage controlled oscillator 4 in the jitter generating circuit 5, the jitter measuring circuit 11 has Since the second phase comparator 7, the second loop filter 8 and the second voltage controlled oscillator 9 are required, there is a drawback that the circuit configuration becomes complicated as the number of components increases. Furthermore, the conventional technique has a problem that it is affected by the nonlinearity of the phase comparator 7 and the loop characteristics of the PLL.

【0007】 この考案はこのような従来技術の欠点を解消し、回路構成を単純にするととも に、位相比較器の非直線性の影響や、PLLのループ特性の影響を受けないジッ タ測定装置を提供することを目的とする。The present invention solves the drawbacks of the prior art, simplifies the circuit configuration, and is not affected by the nonlinearity of the phase comparator or the loop characteristics of the PLL. The purpose is to provide.

【0008】[0008]

【課題を解決するための手段】[Means for Solving the Problems]

この目的を達成するために、この考案では、基準信号21とジッタ信号22を 入力し、これよりジッタを含む被測定信号23を生成するジッタ発生回路5の当 該被測定信号23に含まれるジッタ量を測定するジッタ測定装置は、被測定信号 23を入力し、この被測定信号23を任意の分周比に分周する分周手段11と、 分周手段11より被測定信号23の分周信号24を入力するとともに基準信号2 1を入力し、この基準信号21をトリガ入力として被測定信号23のジッタ量を 測定する測定手段12とを有する。そして、分周手段11で分周される分周比は 被測定信号23のジッタ量に応じて選択される。 In order to achieve this object, according to the present invention, a reference signal 21 and a jitter signal 22 are input and a jitter signal included in the measured signal 23 of a jitter generation circuit 5 that generates a measured signal 23 including jitter is generated. A jitter measuring apparatus for measuring a quantity inputs a signal under measurement 23, divides the signal under measurement 23 to an arbitrary frequency division ratio, and divides the signal under measurement 23 by the frequency dividing means 11. The reference signal 21 is input together with the signal 24, and the reference signal 21 is used as a trigger input to measure the jitter amount of the signal under measurement 23. Then, the division ratio divided by the dividing means 11 is selected according to the amount of jitter of the signal under measurement 23.

【0009】[0009]

【作用】[Action]

この考案によれば、ジッタ発生回路5より出力されたジッタを含む被測定信号 23は分周手段11に送られ、この分周手段11によりジッタ量に応じた分周比 で分周される。測定手段12は、分周手段11で分周された被測定信号23の分 周信号24と、基準信号21を入力し、被測定信号23に含まれるジッタ量の観 測を行う。 According to this invention, the signal to be measured 23 containing the jitter output from the jitter generating circuit 5 is sent to the frequency dividing means 11 and is divided by the frequency dividing means 11 at a frequency dividing ratio according to the amount of jitter. The measuring means 12 inputs the divided signal 24 of the measured signal 23 divided by the dividing means 11 and the reference signal 21, and observes the amount of jitter contained in the measured signal 23.

【0010】[0010]

【実施例】【Example】

次に図1を参照して本考案によるジッタ測定装置の実施例を詳細に説明する。 図1は、本実施例におけるジッタ測定系の構成を示す機能ブロック図である。図 1において、ジッタ発生回路5は、図2に示したジッタ発生回路5と同じ構成要 素を有する同機能の回路である。すなわち、ジッタ発生回路5は、基準信号21 とジッタ信号22を入力し、ジッタ信号22のレベルに比例したジッタ量を持つ 被測定信号23を生成出力する。 Next, an embodiment of the jitter measuring apparatus according to the present invention will be described in detail with reference to FIG. FIG. 1 is a functional block diagram showing the configuration of the jitter measuring system in this embodiment. In FIG. 1, the jitter generating circuit 5 is a circuit having the same structural elements and the same function as the jitter generating circuit 5 shown in FIG. That is, the jitter generating circuit 5 inputs the reference signal 21 and the jitter signal 22, and generates and outputs the signal under measurement 23 having a jitter amount proportional to the level of the jitter signal 22.

【0011】 ジッタ測定装置15は、基準信号21と被測定信号23を入力して、被測定信 号23のジッタ量を測定する装置であり、分周器11とオシロスコープ12によ り構成されている。分周器11は、被測定信号23を入力し、この信号を測定レ ンジに応じて1/N(Nは自然数)に分周する分周器である。分周器11で分周 された被測定信号23は、分周信号24としてオシロスコープ12に送られる。The jitter measuring device 15 is a device for measuring the jitter amount of the signal under measurement 23 by inputting the reference signal 21 and the signal under measurement 23, and is composed of the frequency divider 11 and the oscilloscope 12. There is. The frequency divider 11 is a frequency divider that inputs the signal under measurement 23 and divides this signal into 1 / N (N is a natural number) according to the measurement range. The measured signal 23 divided by the frequency divider 11 is sent to the oscilloscope 12 as a divided signal 24.

【0012】 オシロスコープ12は、分周信号24と基準信号21を入力し、基準信号21 をトリガ入力とすることにより、分周信号24に含まれるジッタ量を測定する測 定器である。本実施例では、被測定信号23が分周器11で1/N分周されるこ とで、N/2周期分より小さいジッタ量がオシロスコープ12を用いて測定でき る。The oscilloscope 12 is a measuring instrument for measuring the amount of jitter contained in the divided signal 24 by inputting the divided signal 24 and the reference signal 21 and using the reference signal 21 as a trigger input. In the present embodiment, the measured signal 23 is divided by 1 / N by the frequency divider 11, so that the amount of jitter smaller than N / 2 cycles can be measured using the oscilloscope 12.

【0013】 次に、図3および図4を用いて図1に示した実施例の動作を説明する。図3は 図1の分周器11の分周比が1/1の場合を示しており、図3(a)は基準信号 21の波形図、図3(b)は被測定信号23の波形図、図3(c)は分周信号2 4の波形図である。Next, the operation of the embodiment shown in FIG. 1 will be described with reference to FIGS. 3 and 4. FIG. 3 shows a case where the frequency division ratio of the frequency divider 11 in FIG. 1 is 1/1. FIG. 3 (a) is a waveform diagram of the reference signal 21 and FIG. 3 (b) is a waveform of the signal under measurement 23. FIG. 3C is a waveform diagram of the divided signal 24.

【0014】 図3(a)の基準信号21と任意な波形のジッタ信号22を受けた図1のジッ タ発生回路5は、ジッタ信号22のレベルに比例したジッタ量を持つ図3(b) の被測定信号23を発生する。The jitter generation circuit 5 of FIG. 1 receiving the reference signal 21 of FIG. 3A and the jitter signal 22 of an arbitrary waveform has a jitter amount proportional to the level of the jitter signal 22 of FIG. 3B. To generate the signal under measurement 23.

【0015】 被測定信号23は、図1の分周器11により分周される。このとき、分周比が 1/1であるので図3(c)の分周信号24は、被測定信号23と同じ信号とな り、基準信号21をトリガ入力としてオシロスコープ12により観測される。The signal under measurement 23 is divided by the frequency divider 11 shown in FIG. At this time, since the frequency division ratio is 1/1, the frequency division signal 24 in FIG. 3C becomes the same signal as the signal under measurement 23 and is observed by the oscilloscope 12 using the reference signal 21 as a trigger input.

【0016】 次に、ジッタ信号22のレベルがさらに大きくなった場合について図4を用い て説明する。図4は、このときの波形図を示したものであり、(a)は基準信号 21の波形図、図4(b)は被測定信号23の波形図、図4(c)は分周信号2 4の波形図をそれぞれ示している。Next, a case where the level of the jitter signal 22 is further increased will be described with reference to FIG. 4A and 4B show waveform diagrams at this time. FIG. 4A is a waveform diagram of the reference signal 21, FIG. 4B is a waveform diagram of the signal under measurement 23, and FIG. 4C is a divided signal. 24 waveform diagrams are shown respectively.

【0017】 ジッタ信号22のレベルを大きくすると、ジッタ発生回路5は図4(b)のよ うな被測定信号23を発生する。このように、ジッタ信号22のレベルが大きい 場合に、被測定信号23を分周比が1/1である分周器11で分周し、オシロス コープ12により観測した場合、図4(b)に示すようにジッタの立ち上がりと 立ち下がりが重なり合いジッタ量を測定することは困難である。そこで、分周器 11の分周比を1/2にして、図4(c)のような分周信号24を得、ジッタ量 の観測を可能とする。When the level of the jitter signal 22 is increased, the jitter generating circuit 5 generates the signal under measurement 23 as shown in FIG. 4B. Thus, when the level of the jitter signal 22 is high, the measured signal 23 is divided by the frequency divider 11 having a division ratio of 1/1 and observed by the oscilloscope 12, as shown in FIG. As shown in, it is difficult to measure the amount of jitter because the rising and falling edges of jitter overlap. Therefore, the frequency division ratio of the frequency divider 11 is halved to obtain the frequency division signal 24 as shown in FIG. 4C, and the jitter amount can be observed.

【0018】 このように、ジッタ量が増加した場合には、分周器11の分周比1/Nを変化 させジッタ量を測定する。このとき、被測定信号23のジッタ量は(τ/T0× 2π)×N[rad]で求めることができる。In this way, when the jitter amount increases, the frequency division ratio 1 / N of the frequency divider 11 is changed to measure the jitter amount. At this time, the amount of jitter of the signal under measurement 23 can be calculated by (τ / T 0 × 2π) × N [rad].

【0019】[0019]

【考案の効果】[Effect of device]

この考案によれば、ジッタ量が増加した場合には分周器11の分周比Nを変化 させて測定信号の重なり合いを取り除くことができ、容易にジッタ量の測定が可 能となる。すなわち、本考案では、ジッタ発生回路5で発生させたジッタを含む 信号は、被測定信号23を分周手段11で1/Nに分周することによってN/2 周期分より小さいジッタ量を測定手段12で簡単に測定することができる。 According to this invention, when the amount of jitter increases, the frequency division ratio N of the frequency divider 11 can be changed to remove the overlap of the measurement signals, and the amount of jitter can be easily measured. That is, in the present invention, the signal including the jitter generated by the jitter generating circuit 5 is divided into 1 / N by the frequency dividing means 11 to measure the jitter amount smaller than N / 2 cycles. It can be easily measured by means 12.

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

【図1】本考案によるジッタ測定装置の実施例を示す機
能ブロック図である。
FIG. 1 is a functional block diagram showing an embodiment of a jitter measuring apparatus according to the present invention.

【図2】従来技術によるジッタ測定系の構成例である。FIG. 2 is a configuration example of a jitter measuring system according to a conventional technique.

【図3】図1の実施例を説明するための波形図である。FIG. 3 is a waveform diagram for explaining the embodiment of FIG.

【図4】図1の実施例を説明するための波形図である。FIG. 4 is a waveform diagram for explaining the embodiment of FIG.

【符号の説明】[Explanation of symbols]

5 ジッタ発生回路 11 分周器 12 オシロスコープ 21 基準信号 22 ジッタ信号 23 被測定信号 24 分周信号 5 Jitter generation circuit 11 Divider 12 Oscilloscope 21 Reference signal 22 Jitter signal 23 Signal under test 24 Divided signal

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 【請求項1】 基準信号(21)とジッタ信号(22)を入力
し、これよりジッタを含む被測定信号(23)を生成するジ
ッタ発生回路(5) の当該被測定信号(23)に含まれるジッ
タ量を測定するジッタ測定装置において、 前記被測定信号(23)を入力し、この被測定信号(23)を任
意の分周比に分周する分周手段(11)と、 前記分周手段(11)より前記被測定信号(23)の分周信号(2
4)を入力するとともに前記基準信号(21)を入力し、この
基準信号(21)をトリガ入力として前記被測定信号(23)の
ジッタ量を測定する測定手段(12)とを有し、 前記分周手段(11)で分周される分周比は前記被測定信号
(23)のジッタ量に応じて選択されることを特徴とするジ
ッタ測定装置。
1. A signal to be measured (23) of a jitter generation circuit (5) for inputting a reference signal (21) and a jitter signal (22) to generate a signal to be measured (23) including jitter. In the jitter measuring device for measuring the amount of jitter, the signal under measurement (23) is input, and the frequency dividing means (11) for dividing the signal under measurement (23) to an arbitrary frequency division ratio is used. From the means (11), the frequency-divided signal (2
4) and the reference signal (21) is input, and the reference signal (21) as a trigger input and has a measuring means (12) for measuring the amount of jitter of the signal under measurement (23), The dividing ratio divided by the dividing means (11) is the signal under measurement.
A jitter measuring device characterized by being selected according to the amount of jitter of (23).
JP7140292U 1992-09-18 1992-09-18 Jitter measuring device Pending JPH0628753U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP7140292U JPH0628753U (en) 1992-09-18 1992-09-18 Jitter measuring device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7140292U JPH0628753U (en) 1992-09-18 1992-09-18 Jitter measuring device

Publications (1)

Publication Number Publication Date
JPH0628753U true JPH0628753U (en) 1994-04-15

Family

ID=13459490

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7140292U Pending JPH0628753U (en) 1992-09-18 1992-09-18 Jitter measuring device

Country Status (1)

Country Link
JP (1) JPH0628753U (en)

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