Thanks to all who replied, and sorry for the delay. I was away and unfortunately unable to follow the discussion until today.
From Tom's comments and others I extract that the PM6681 can only be used for measuring the ADEV when employing the picket fence technique. A direct measurement is prevented by the counter's dead-time. Apart from a suitable divider, I'd probably need to write my own piece of software for massaging the data so that it can be used for an ADEV plot. Unless of course there is some software readily available that includes handling of the picket fence technique.
My other idea of using two counters in lockstep, so that they measure alternate periods of the signal, hasn't been commented on. Is it a silly idea, apart from the fact that it needs two counters? Has anyone tried anything like it?
Thanks and Cheers
Stefan
-----Ursprüngliche Nachricht-----
Von: time-nuts-bounces@febo.com [mailto:time-nuts-bounces@febo.com] Im Auftrag von Tom Duckworth
Gesendet: Samstag, 25. Oktober 2008 03:11
An: 'Discussion of precise time and frequency measurement'
Betreff: Re: [time-nuts] Measuring ADEV with a PM6681 or CNT-81
Stefan,
Well, I have been sort of staying out of the recent discussions regarding
oscillator stability measurements, ADEV, etc., but here goes my two cents
worth. I hope it doesn't muddy the waters too much and is somewhat helpful.
There is a fundamental problem with trying to do ADEV (Allan Deviation) with
a counter that has a gated measurement engine (all standard counters). The
problem is that when the count engine gate closes (so the counter can
compute the number of events, report the result as a frequency, and clear
its registers), the counter is blind (dead time) to any signal at the input.
Allan deviation REQUIRES than a minimum number of measurements be made
back-to-back (no dead time between measurements) in order to capture
nondeterministic fluctuations of the signal you're trying to measure. This
requires a measuring device (counter) that continuously records ALL events.
It does this by time-stamping a fixed period in a separate register in the
counter along with the input register (the signal being measured), and a
time-base register that records the frequency the signal is to be compared
with. There is no 'gate' as such in a time-stamping counter.
Most stability measurements, longer than say 100 seconds, are made in the
frequency domain because energy changes, as a result of heat, are by far the
predominate cause of stability (aging) issues (see below). Stability issues
within shorter time periods, say <100 sec., are often nondeterministic, and
cannot be accurately quantified in the frequency domain, but must be
measured in the time domain, using statistical weighting. In other words,
unpredictable, and often little understood, events (Shot and thermal noise
in the active devices, random variations in the frequency-determining
elements, cosmic rays, etc.) often predominate short term stability
measurements and must be described statistically, as their occurrence and
duration are random. Allan deviation is a widely accepted time-domain
statistical measurement whose calculated results compare well with the more
common frequency domain measurement of longer time periods.
Allan deviation measurements are based on the sample variance of the
fractional-frequency fluctuations. Without specifying the number of samples
N, and the repetition interval T, for measurements of duration t, the
measure of frequency stability is dimensionless and would converge to a
meaningless limit. Secondly, some actual noise processes contain substantial
fractions of the total noise power in the instantaneous fractional-frequency
range below one cycle per year. In order to improve compatibility of data,
it is important to specify a particular N and T. The Allan variance chooses
N=2 and T=t (i.e. no dead time between measurements). A good estimate can be
obtained by a limited number, m, of measurements (m=*100). Root Allen
variance is expressed as a quantity divided by the square of the
measurements of duration t, (i.e., 3 x 10-11/*t).
.
Classical variance diverges for commonly observed noise processes, such as
random walk (i.e., the variance increases with an increasing number of data
points). The advantage with the Allan variance is that it:
converges for all noise processes observed in precision
oscillators;
has straightforward relationship to power law spectral density
(spectral density of the frequency fluctuations);
is easy to compute, and;
is faster and more accurate in estimating noise processes than
the Fast Fourier Transform.
Aging in quartz crystal oscillators is caused by changes in either the
quartz crystal itself or the associated components found in the oscillator
assembly. Aging is the result of a combination of several factors having
complex, and only partially understood, components that effect the aging
specification. Effects can include the cut (orientation) of the crystal;
vibration modes; frequency of cut size; temperature of operation and
variations of temperature; drive energy; gravity; physical orientation;
shock; electromagnetic interference; diffusion of impurities and the
outgassing of the quartz crystal; the glass or ceramic base; the adhesive
used to mount the quartz; metal migration from the electrodes into the
quartz surface; stress relief of the crystal mounts; changes of electric
component values over time; and, voltage regulation.
This is probably more information than you really wanted, but oh well,
enjoy.
Tom
Tom Duckworth
510-886-1396
-----Original Message-----
From: time-nuts-bounces@febo.com [mailto:time-nuts-bounces@febo.com] On
Behalf Of Heinzmann, Stefan (ALC NetworX GmbH)
Sent: Friday, October 24, 2008 2:03 AM
To: Discussion of precise time and frequency measurement
Subject: Re: [time-nuts] Measuring ADEV with a PM6681 or CNT-81
Thanks, Tom!
Apart from the specifics with TimeView, how does one go about measuring ADEV
with a counter that does have a dead-time? Are there tricks that can be
played, either with a special measurement setup or with some data
postprocessing? Or with two counters that are somehow made to cooperate?
Sorry if I'm asking the obvious, you can see that I'm a greenhorn. ;-)
Cheers
Stefan
-----Ursprüngliche Nachricht-----
Von: time-nuts-bounces@febo.com [mailto:time-nuts-bounces@febo.com] Im
Auftrag von Tom Duckworth
Gesendet: Donnerstag, 23. Oktober 2008 22:19
An: 'Discussion of precise time and frequency measurement'
Betreff: Re: [time-nuts] Measuring ADEV with a PM6681 or CNT-81
Stefan,
I am retired from Pendulum Instruments and could answer your question but I
have instead refered your question to a current engineer with the company
and you should receive an answer from them shortly. They are the experts for
this question.
Tom
Tom Duckworth
510-886-1396
-----Original Message-----
From: time-nuts-bounces@febo.com [mailto:time-nuts-bounces@febo.com] On
Behalf Of Heinzmann, Stefan (ALC NetworX GmbH)
Sent: Thursday, October 23, 2008 10:12 AM
Subject: [time-nuts] Measuring ADEV with a PM6681 or CNT-81
Hi all,
I hope you can clear up some confusion that I have regarding ADEV
measurement. I was under the impression that you need a counter that is able
to timestamp each rising edge of the clock under test, or equivalently
measure period time continuously with no dead time. Now, while the CNT-90
can do this, the CNT-81 ( = PM6681 ) can't. Still, a message last December
to the list here
(http://www.mail-archive.com/time-nuts@febo.com/msg10963.html) seems to
indicate that using TimeView you can have ADEV plotted with the "lesser"
model, too. I have a PM6681 and TimeView, but I couldn't find out how to do
it. Maybe it can't be done.
So what's the deal on this? Can it be done, with or without TimeView, and if
yes, how? If this has been answered earlier, a link would be just fine.
Thanks and cheers
Stefan
time-nuts mailing list -- time-nuts@febo.com
To unsubscribe, go to
https://www.febo.com/cgi-bin/mailman/listinfo/time-nuts
and follow the instructions there.
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To unsubscribe, go to
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and follow the instructions there.
Stefan,
Apart from a suitable divider, I'd....
If you a dedicated follower of PIC microcontrollers you find something
suitable here on Tom's pages
http://www.leapsecond.com/pages/ppsdiv/
Otherwise if you like AVRs then you can find something on my pages
http://www.ulrich-bangert.de/html/downloads.html
Suitable sine to ttl circuits designed by Bruce Griffiths are to be
found at
http://www.ko4bb.com/~bruce/CLKSHPR.html
Best regards
Ulrich
-----Ursprüngliche Nachricht-----
Von: time-nuts-bounces@febo.com
[mailto:time-nuts-bounces@febo.com] Im Auftrag von Heinzmann,
Stefan (ALC NetworX GmbH)
Gesendet: Donnerstag, 30. Oktober 2008 12:42
An: Discussion of precise time and frequency measurement
Betreff: [!! SPAM] Re: [time-nuts] Measuring ADEV with a
PM6681 or CNT-81
Thanks to all who replied, and sorry for the delay. I was
away and unfortunately unable to follow the discussion until today.
From Tom's comments and others I extract that the PM6681 can
only be used for measuring the ADEV when employing the picket
fence technique. A direct measurement is prevented by the
counter's dead-time. Apart from a suitable divider, I'd
probably need to write my own piece of software for massaging
the data so that it can be used for an ADEV plot. Unless of
course there is some software readily available that includes
handling of the picket fence technique.
My other idea of using two counters in lockstep, so that they
measure alternate periods of the signal, hasn't been
commented on. Is it a silly idea, apart from the fact that it
needs two counters? Has anyone tried anything like it?
Thanks and Cheers
Stefan
-----Ursprüngliche Nachricht-----
Von: time-nuts-bounces@febo.com
[mailto:time-nuts-bounces@febo.com] Im Auftrag von Tom Duckworth
Gesendet: Samstag, 25. Oktober 2008 03:11
An: 'Discussion of precise time and frequency measurement'
Betreff: Re: [time-nuts] Measuring ADEV with a PM6681 or CNT-81
Stefan,
Well, I have been sort of staying out of the recent
discussions regarding oscillator stability measurements,
ADEV, etc., but here goes my two cents worth. I hope it
doesn't muddy the waters too much and is somewhat helpful.
There is a fundamental problem with trying to do ADEV (Allan
Deviation) with a counter that has a gated measurement engine
(all standard counters). The problem is that when the count
engine gate closes (so the counter can compute the number of
events, report the result as a frequency, and clear its
registers), the counter is blind (dead time) to any signal at
the input. Allan deviation REQUIRES than a minimum number of
measurements be made back-to-back (no dead time between
measurements) in order to capture nondeterministic
fluctuations of the signal you're trying to measure. This
requires a measuring device (counter) that continuously
records ALL events. It does this by time-stamping a fixed
period in a separate register in the counter along with the
input register (the signal being measured), and a time-base
register that records the frequency the signal is to be
compared with. There is no 'gate' as such in a time-stamping counter.
Most stability measurements, longer than say 100 seconds, are
made in the frequency domain because energy changes, as a
result of heat, are by far the predominate cause of stability
(aging) issues (see below). Stability issues within shorter
time periods, say <100 sec., are often nondeterministic, and
cannot be accurately quantified in the frequency domain, but
must be measured in the time domain, using statistical
weighting. In other words, unpredictable, and often little
understood, events (Shot and thermal noise in the active
devices, random variations in the frequency-determining
elements, cosmic rays, etc.) often predominate short term
stability measurements and must be described statistically,
as their occurrence and duration are random. Allan deviation
is a widely accepted time-domain statistical measurement
whose calculated results compare well with the more common
frequency domain measurement of longer time periods.
Allan deviation measurements are based on the sample variance
of the fractional-frequency fluctuations. Without specifying
the number of samples N, and the repetition interval T, for
measurements of duration t, the measure of frequency
stability is dimensionless and would converge to a
meaningless limit. Secondly, some actual noise processes
contain substantial fractions of the total noise power in the
instantaneous fractional-frequency range below one cycle per
year. In order to improve compatibility of data, it is
important to specify a particular N and T. The Allan variance
chooses N=2 and T=t (i.e. no dead time between measurements).
A good estimate can be obtained by a limited number, m, of
measurements (m=*100). Root Allen variance is expressed as a
quantity divided by the square of the measurements of
duration t, (i.e., 3 x 10-11/*t).
.
Classical variance diverges for commonly observed noise
processes, such as random walk (i.e., the variance increases
with an increasing number of data points). The advantage with
the Allan variance is that it:
converges for all noise processes observed in precision
oscillators;
has straightforward relationship to power law
spectral density
(spectral density of the frequency fluctuations);
is easy to compute, and;
is faster and more accurate in estimating noise
processes than
the Fast Fourier Transform.
Aging in quartz crystal oscillators is caused by changes in
either the quartz crystal itself or the associated components
found in the oscillator assembly. Aging is the result of a
combination of several factors having complex, and only
partially understood, components that effect the aging
specification. Effects can include the cut (orientation) of
the crystal; vibration modes; frequency of cut size;
temperature of operation and variations of temperature; drive
energy; gravity; physical orientation;
shock; electromagnetic interference; diffusion of impurities
and the outgassing of the quartz crystal; the glass or
ceramic base; the adhesive used to mount the quartz; metal
migration from the electrodes into the quartz surface; stress
relief of the crystal mounts; changes of electric component
values over time; and, voltage regulation.
This is probably more information than you really wanted, but
oh well, enjoy.
Tom
Tom Duckworth
510-886-1396
-----Original Message-----
From: time-nuts-bounces@febo.com
[mailto:time-nuts-bounces@febo.com] On Behalf Of Heinzmann,
Stefan (ALC NetworX GmbH)
Sent: Friday, October 24, 2008 2:03 AM
To: Discussion of precise time and frequency measurement
Subject: Re: [time-nuts] Measuring ADEV with a PM6681 or CNT-81
Thanks, Tom!
Apart from the specifics with TimeView, how does one go about
measuring ADEV with a counter that does have a dead-time? Are
there tricks that can be played, either with a special
measurement setup or with some data postprocessing? Or with
two counters that are somehow made to cooperate?
Sorry if I'm asking the obvious, you can see that I'm a greenhorn. ;-)
Cheers
Stefan
-----Ursprüngliche Nachricht-----
Von: time-nuts-bounces@febo.com
[mailto:time-nuts-bounces@febo.com] Im Auftrag von Tom Duckworth
Gesendet: Donnerstag, 23. Oktober 2008 22:19
An: 'Discussion of precise time and frequency measurement'
Betreff: Re: [time-nuts] Measuring ADEV with a PM6681 or CNT-81
Stefan,
I am retired from Pendulum Instruments and could answer your
question but I
have instead refered your question to a current engineer with
the company
and you should receive an answer from them shortly. They are
the experts for
this question.
Tom
Tom Duckworth
510-886-1396
-----Original Message-----
From: time-nuts-bounces@febo.com
[mailto:time-nuts-bounces@febo.com] On
Behalf Of Heinzmann, Stefan (ALC NetworX GmbH)
Sent: Thursday, October 23, 2008 10:12 AM
Subject: [time-nuts] Measuring ADEV with a PM6681 or CNT-81
Hi all,
I hope you can clear up some confusion that I have regarding ADEV
measurement. I was under the impression that you need a
counter that is able
to timestamp each rising edge of the clock under test, or equivalently
measure period time continuously with no dead time. Now,
while the CNT-90
can do this, the CNT-81 ( = PM6681 ) can't. Still, a message
last December
to the list here
(http://www.mail-archive.com/time-nuts@febo.com/msg10963.html)
seems to
indicate that using TimeView you can have ADEV plotted with
the "lesser"
model, too. I have a PM6681 and TimeView, but I couldn't find
out how to do
it. Maybe it can't be done.
So what's the deal on this? Can it be done, with or without
TimeView, and if
yes, how? If this has been answered earlier, a link would be
just fine.
Thanks and cheers
Stefan
time-nuts mailing list -- time-nuts@febo.com
To unsubscribe, go to
https://www.febo.com/cgi-bin/mailman/listinfo/time-nuts
and follow the instructions there.
time-nuts mailing list -- time-nuts@febo.com
To unsubscribe, go to
https://www.febo.com/cgi-bin/mailman/listinfo/time-nuts
and follow the instructions there.
time-nuts mailing list -- time-nuts@febo.com
To unsubscribe, go to
https://www.febo.com/cgi-bin/mailman/listinfo/time-nuts
and follow the instructions there.
time-nuts mailing list -- time-nuts@febo.com
To unsubscribe, go to
https://www.febo.com/cgi-bin/mailman/listinfo/time-nuts
and follow the instructions there.
time-nuts mailing list -- time-nuts@febo.com
To unsubscribe, go to
https://www.febo.com/cgi-bin/mailman/listinfo/time-nuts
and follow the instructions there.
Apart from a suitable divider
And I have one PCB left for my divider if that's of interest ... Price as
before GBP20 plus shipping (GBP12 outside UK) plus 5% Paypal tax!
PS has anyone had a chance to measure the phase noise from my divider yet -
I just don't have the tools to do it, and I know that a few of you suggested
you'd look at that after building it.
Cheers
Dave
-----Original Message-----
From: time-nuts-bounces@febo.com [mailto:time-nuts-bounces@febo.com] On
Behalf Of Heinzmann, Stefan (ALC NetworX GmbH)
Sent: 30 October 2008 11:42
To: Discussion of precise time and frequency measurement
Subject: Re: [time-nuts] Measuring ADEV with a PM6681 or CNT-81