Hi

More or less in order:

The beat frequency is coming out of a rubidium. Hopefully it's fairly stable. 
It won't be super quiet for 1 or .1 second tau. It looks like the counter will 
be a FPGA time tagger, so the beat note frequency will drop out for free. 

The isolation amps are common base buffers. Not much gain, but quite a bit of 
isolation. Phase shift / C - need to look into that.

Mixer loading likely would be as I've done it before. Resistive termination at 
RF and fairly high impedance at audio. Resistor here and there to improve the 
match at RF. LC filtering adequate to suppress the RF stuff on the output of 
the mixer.  Single pole R-C for audio bandwidth control. Big capacitors and 
small resistors for low noise. 

Until I've measured them I'm not sure of the floor of the limiters. Before I 
get into that I want to be fairly sure I'm not over spec'ing them. If 100 ns is 
as good as 3 ns it's not as hard a problem. 

The issue of the group delay is an interesting one. I believe that people have 
been getting good results with coax line for the phase shift. I'm a bit 
conflicted on the  coax. 15 meters of small diameter stuff will fit in the box 
(maybe), but it's not super stable.. If I go foam coax then the phase shifter 
gets pretty big. If I go with some kind of LC setup, temperature stability 
would likely be an issue. 

Crazy Stuff ....

So what did I miss that time?

Bob



 
On Jan 24, 2010, at 9:01 PM, Magnus Danielson wrote:

> Bob Camp wrote:
>> Hi
>> I realize that this is a bit off topic from the flow of the last few days. I 
>> can only claim temporary insanity. Any comments about the temporary modifier 
>> in that sentence being unneeded will of course be ignored...
>> Assuming that:
>> 1) I have a DMTD setup of the "basement engineering" variety.
>> 2) The beat note is > 5 Hz and < 10 Hz
>> 3) The DUT's are all worse than 1x10^-12 at one second tau (no hydrogen 
>> masers in the basement)
>> 4) The offset oscillator is at least 2x10^-11 at one second tau.
>> 5) The DUT's all put out 10 MHz
>> 6) My counter will resolve 10 ns (= I could do better)
>> 7) The limiters are good enough to not be an issue relative to the counter's 
>> 10 ns.
>> 8) The zero crossings are phase shifted to be close, but not so close I arm 
>> after I start during a run. 9) Regardless of the tau involved, nothing I'm 
>> looking at will be better than 1x10-14
>> My down conversion from 10 MHz to 10 Hz gives me a 10^6 multiplication.
>> 10 ns is a part in 10^8 at one second. It's a part in 10^7at 0.1 second (10 
>> Hz).
>> First order, I should be able to hit (7+6 = 13) a part in 10^13 at less than 
>> 1 second. That's significantly better than the DUT's. I don't need anything 
>> better in the counter or limiters to measure what I'm looking at. Even if 
>> the limiters are 2X worse than the counter, I'm still at the don't need 
>> better level in terms of counter and limiters. The offset oscillator is 
>> going to cause some second order issues regardless of the limiters and 
>> counter, but it still should be "ok". Next up:
>> If I phase shift one of the DUT's by 360 degrees, the beat note does the 
>> same. All I need is 100 ns of phase shift to get everything lined up. I 
>> could do it with 180 degrees of shift and an phase inversion switch. I'm 
>> assuming (phase shifter and DMTD stuff)  can fit it all in a 2x4x8" box - I 
>> don't need a new bench to hold it all ...
>> So what did I miss? 
> 
> Remember that you *must* measure the actual beat frequency, since you will 
> need that to calculate the beat-gain. If it is between 5 and 10 Hz
> the for a 10 MHz source your gain is 2E6 and 1E6 respectively, which is a 
> factor of 2 difference or 6 dB. So, your measurements will be inprecise from 
> that factor alone by +/- 3 dB. The remedy is fairly easy to come up with, 
> measure the input frequency and beat frequency for each arm. The best thing 
> is naturally to ensure that the beat frequencies of both arms is fairly 
> close. EFC steering of either source may work well enought in open-loop mode 
> during measurement (with the added benefit of not do spectral interference 
> with the phase noise which locked loop does).
> 
> How do you control the input levels to the mixers?
> 
> Do you have any isolational amplifiers?
> 
> How do you load and pre-filter the mixer outputs?
> 
> You haven't convinced me of the expected performance of the limiters.
> 
> I'm not sure it will be your biggest problem, but the way you phase-shift can 
> be of importance for the decorrelation loss.
> Phase-shifting such that group-delay moves noise in time will be problematic, 
> since then the decorrelation gain of having phases coincide  will be partly 
> lost since it is the group-delayed variant of the transfer oscillator against 
> the current-time transfer-oscillator (both delayed by each detector arm, but 
> only differnces is important). Vector-adding phase delays could work around 
> that. The optimum delay setting for cancelation may not be to fully 
> phase-adjust the leading edge.
> 
> That is what just popped up in my head at least.
> 
> Cheers,
> Magnus
> 
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