Hi,

On 2020-02-29 23:10, Taka Kamiya via time-nuts wrote:
> One question for Magnus.
>
> Ch A start - pps (standard)Ch B stop - DUT
> On item 4, you said "frequency of the signal on time B".  That much is 
> obvious.  But then you said: "give it the time-base of the period on the 
> A-channel".  Will you explain this?
> Say I give 1 Hz, period is 1s.  Say I give 10Hz, period is 0.1s.  Is this 
> what you mean?
Yes. Exactly.
> I'm using HP5370A.  This instruction is valid on this TI counter, correct??
Yes. It will work.
>
> A request for everyone:
> I am conducting an one hour measurement on HP105B.  Does anyone have 1 hour 
> plot of this signal generator handy?  If so, will you DM me a copy?  For some 
> reason, I cannot find one on the great Internet.

I have one of the 00105 oscillator ,as mounted and free-running in a
HP5065A, against hydrogen maser at hand. I can locate that and send you
if you wish. It's longer than 1 hour, but you get additional precision
from this.

Cheers,
Magnus

>
> ------------------- clip from Magnus's previous email------------------
> A setup I use a lot is this:
> 1) Connect a reference oscillator to produce a 1 Hz or 10 Hz signal and
> feed into a counter Channel A/TI-start channel. For PPS signals, I make
> sure to trigger a but up on the rising edge not to false-trigger. For
> some counters this means turning of automatic trigger and set it to 1 V
> manually. It is important that no false triggers occurs.
>
> 2) Connect a signal under test to Channel B/TI-stop. Adjust trigger to
> through-zero or up on the edge as suitable.
>
> 3) TI-mode, continuous trigger
>
> 4) Collect data in TimeLab, give TimeLab the frequency of the signal on
> B-channel, give it the time-base of the period on the A-channel.
>
> 5) Look at data as it comes in. Look at phase view, frequency view,
> wrapped phase. Look at the ADEV, how the upper end flaps with data, but
> how the same tau becomes more and more stable as it comes 
> in.---------------------
> --------------------------------------- 
> (Mr.) Taka Kamiya
> KB4EMF / ex JF2DKG
>  
>
>     On Friday, February 21, 2020, 9:26:47 PM EST, Magnus Danielson via 
> time-nuts <time-nuts@lists.febo.com> wrote:  
>  
>  Hi Taka,
>
> On 2020-02-21 23:26, Taka Kamiya via time-nuts wrote:
>> I'm sorry, I messed up.  I jumped on more advance topic than I intended.  
>> I'm sure there were answers in the replies but they must have gone way over 
>> my head because some of original questions still remain.  I bulletized (is 
>> that a word?) the original question with my NEW understanding.  Would 
>> someone please respond for me, point-to-point?
> No problem. No worries. I hope you end up reading these and the other
> replies again and acquire good knowledge. I know it's like drinking from
> a fire-hoze, but you did ask some very relevant and fair questions.
>> 1)  A frequency counter that measures DUT basically puts out a reading every 
>> second during the measurement.  When TimeLab is well into 1000s or so, it is 
>> still reading every second; it does not change the gate time to say, 1000s.  
>> I understand now, Adev is about phase, not the frequency.  But assuming DUT 
>> is sine wave, if there is enough phase change, frequency do change.  I think 
>> of phase change as frequency change that is less than full cycle.  So how 
>> does counters that outputs every 1 second end up in tau of 1000s?  It will 
>> entirely miss phase change that spans more than 1 cycle.
> ADEV is about the frequency stability. ADEV can be calculated using
> phase or frequency measures. We tend to prefer using phase measures from
> Time-Interval Counters for these things.
>
> OK, so let's say that we want to output a counter which provides output
> of frequency estimates but for a time-base which is longer than 1 s,
> even if we output results every 1 s?
>
> Classically counters could not do that. You acquired a start-value,
> waited the time-base, acquired a stop-value, calculated a result to
> display and then arm to get a new start-value for the next result. Such
> counters will have a limit that the rate of readings will be limited by
> the time-base, so if it is set to 10 s, only every 10 s and output is
> produced.
>
> To tackle this, one needs a counter that can interleave frequency
> measurements, so that it generates new start-points at the update rate
> even if the stop-point has not occurred. So, for a time-base of 10 s and
> an update rate of 1 s, then every 1 s a new start-trigger is produced,
> and then remembered until a stop trigger can be produced, at which time
> the start-trigger 10 s back is used to estimate the frequency. In fact,
> for this to work, the stop trigger time-stamp is also the start trigger
> time-stamp for a new measurement. You can do this with any time-base
> really, and the degree of interleaving only depends on the number of
> start-points one can keep in memory.
>
>> 2)  I recall reading on TICC manual, in time interval mode, anything that's 
>> reasonably good is good enough, because it has time stamp and the count 
>> reading.  Clock is used to chunk the data.  Is this still true?  Through 
>> this discussion, I ended up with conclusion that there is no inherent 
>> advantage over TI measurement when compared to frequency measurement.  Am I 
>> understanding this correctly?
> There is benefits in time-measures over frequency measures when one
> monitors long-term properties. Also, as one tries to create a
> phase-curve from frequency estimates, any rounding off errors show in an
> slope, as there is a tiny average frequency offset from round-offs. Only
> really good such setups does not have significant slope.
>
>> 3)  I understand even the BEST counter is only good for Adev nE-12 
>> measurement. Then, with my collection of counters, HP53132A (which averages 
>> tons of short period measurement), 5335A (not enough resolution), HP5370A 
>> (interval reading is no better than frequency), TICC by TAPR,   Do I even 
>> have a chance of doing any meaningful work?  (say work with GPSDO and Rb 
>> which some of it does reach E-13)  Yes, I know now, it is NOT possible to do 
>> 1 sec Adev but say over 100 seconds?  Right now, I don't have any standard 
>> that has adev that good at 1 sec anyway.
> The resolution of your counter tells you about where your 1/tau curve
> will cut tau = 1 s, and it goes from there. There is a slight scaling
> factor, but if we assume it is 1 for now, it is pretty simple. Your
> 5335A has 1 ns single-shot resolution, this gives 1E-9 at 1 s, but 1E-10
> at 10 s, 1E-11 at 100 s and 1E-12 at 1000 s. You see very clearly when
> the linear slope ends and "lands" in the noise, at which time the noise
> becomes dominant and is giving you the interesting reading. The 5370A is
> 20 ps single-shot resolution, giving you a whopping 2E-11 at 1 s, 2E-12
> at 10 s, 2E-13 at 100 s and 2E-14 at 1000 s. It's some serious
> improvement. You are more likely to be limited by your oscillators as
> ref and under test at 1000 s with that one, than the instrument itself.
>
>> 4)  Would one person who has infinite patience and experience guide me 
>> through getting one reading done correctly with what I already have?  That 
>> may include email and phone call.  (I speak English and Japanese)  I don't 
>> want to lower S/N of this mailing list by doing this here.  
> I think you have contributed by asking some really good questions.
>
> A setup I use a lot is this:
>
> 1) Connect a reference oscillator to produce a 1 Hz or 10 Hz signal and
> feed into a counter Channel A/TI-start channel. For PPS signals, I make
> sure to trigger a but up on the rising edge not to false-trigger. For
> some counters this means turning of automatic trigger and set it to 1 V
> manually. It is important that no false triggers occurs.
>
> 2) Connect a signal under test to Channel B/TI-stop. Adjust trigger to
> through-zero or up on the edge as suitable.
>
> 3) TI-mode, continuous trigger
>
> 4) Collect data in TimeLab, give TimeLab the frequency of the signal on
> B-channel, give it the time-base of the period on the A-channel.
>
> 5) Look at data as it comes in. Look at phase view, frequency view,
> wrapped phase. Look at the ADEV, how the upper end flaps with data, but
> how the same tau becomes more and more stable as it comes in.
>
> Using even old counters this setup have helped a lot for many measures.
> It is simple and sturdy for many measures. Remember to save traces, to
> annotate it carefully so one can understand afterwards what one did.
>
> Using this setup, I swapped a HP53132A (150 ps) for a HP5335A (1 ns) and
> then PM6853A (2 ns) to show that a particular problem did not needed the
> best counter in the house to be well characterized.
>
>> 5)  One time, it was mentioned many of Adev graphs posted are basically a 
>> graph of instruments noise graph.  How do I tell when a given reading/graph 
>> is exceeding the limit of a setup?  I did do base line where same signal 
>> goes to counter's reference input and signal input.  I always have that on 
>> my chart so traces does not go below.  Is that enough?
> Almost. It's a good start. The first slope for lower taus is due to the
> instrument for sure. If you look carefully you will notice that the
> actual performance shifts around, because it is more complex than just
> being instrument limit, but it is the right ball-park for that part of
> the plots. For the upper end, you can be limited by your device under
> test drift. This can be handled by simply letting them be turned on
> longer. Sub-sequent measurement will have that rising slope move more
> and more towards higher taus and thus becomming less like a limit-issue
> for a certain tau.
>> I appreciate everyone's input.  I am learning a lot but just not digesting 
>> well enough.  I'd like to do DMTD after I understand the basics.
> Good spirit. DMTD takes some care, but once you learned it, it can be a
> magnificent tool.
>
> Cheers,
> Magnus
>
>> --------------------------------------- 
>> (Mr.) Taka Kamiya
>> KB4EMF / ex JF2DKG
>>   
>>
>>     On Thursday, February 20, 2020, 1:41:06 PM EST, Taka Kamiya via 
>> time-nuts <time-nuts@lists.febo.com> wrote:  
>>   
>>   I have a question concerning frequency standard and their Allen deviation. 
>>  (to measure Allen Dev in frequency mode using TimeLab)
>>
>> It is commonly said that for shorter tau measurement, I'd need OCXO because 
>> it's short tau jitter is superior to just about anything else.  Also, it is 
>> said that for longer tau measurement, I'd need something like Rb or Cs which 
>> has superior stability over longer term.
>> Here's the question part.  A frequency counter that measures DUT basically 
>> puts out a reading every second during the measurement.  When TimeLab is 
>> well into 1000s or so, it is still reading every second; it does not change 
>> the gate time to say, 1000s.
>> That being the case, why this consensus of what time source to use for what 
>> tau?
>> I recall reading on TICC, in time interval mode, anything that's reasonably 
>> good is good enough.  I'm aware TI mode and Freq mode is entirely different, 
>> but it is the same in fact that measurement is made for very short time span 
>> AT A TIME.
>> I'm still trying to wrap my small head around this.  
>>
>> --------------------------------------- 
>> (Mr.) Taka Kamiya
>> KB4EMF / ex JF2DKG
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