Hi,

If you have a GPSDO, then PPS as re-generated from the locked oscillator
is naturally less noisy than straight from the GPS. Using a PICDIV helps
you to use another reference instead, and the TADD-2 is a useful option
to consider.

I have my TADD-2:s modified such that one of the outputs is the input
clock buffered, which is a simple wire from the clock input of the PIC
over to one of the output drivers. This gives better jitter performance
than feeding a 5 MHz or 10 MHz sine straight into a TIC channel.

However, the important is that you start measure. Even somewhat
imperfect measures is better than nothing, and taking several measures
as you do, I think you will see a pattern re-emerge in them as being the
tell-tail of your measurement limits. Consider that single-shot
resolution and white noise has a 1/tau slope on them, so eventually you
go down to the combination of the actual DUT and GPS noise, rather than
that of the PPS placement.

Cheers,
Magnus

On 2020-03-01 01:25, Taka Kamiya via time-nuts wrote:
> YES, please.  [email protected].
> So far, I've taken HP105B and did adev frequency reading based, T.I. based 
> adev, and while at it, I am doing PRS-10 T.I. based.
> I have a question.  My 1 second reference for channel A is coming from GPS 
> based 1 second.  I understand it's only 10E-8 precision on second to second 
> basis?  Is this sufficient for OCXO and Rb based oscillators?
>
> --------------------------------------- 
> (Mr.) Taka Kamiya
> KB4EMF / ex JF2DKG
>  
>
>     On Saturday, February 29, 2020, 7:21:28 PM EST, Magnus Danielson 
> <[email protected]> wrote:  
>  
>  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 <[email protected]> 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 <[email protected]> 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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