Hi

Again more or less in order:

I'm trying to keep things as simple as I can at least to start. That rules out 
the clean up loop oscillator at least in the beginning. It is a good idea, and 
eventually I'll probably put one in.

I guess I'm going to need to do some looking on transformer feedback high 
isolation amps. Everything I've seen so far on hight isolation has been 
straight / no feedback stuff.

The loading at RF on the mixer does reduce the audio output, but it improves 
the isolation / match on the mixer. You trade one for the other.

Looks like some kind of local temperature stabilization might be a good idea 
for the audio band limiting stuff. It's after the down convert, but some of the 
time constants are indeed very long. 

I suspect that silica dielectric cable is outside the budget constraints on 
this project. Cheap foam coax in a spool on the floor or tiny stuff in the box, 
possibly with better temperature control are about the only two choices. 

---------

Another very real choice is to simply move the goal post a bit. Pushing the 
1x10*-12 point to 10 seconds from 1 second could turn out to be the only 
economical basement alternative.

Off to bed ....

Bob

On Jan 24, 2010, at 10:26 PM, Bruce Griffiths wrote:

> Bob Camp wrote:
>> 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.
>> 
>>   
> A cleanup loop may be useful to improve the offset source short term 
> stability.
> The cancellation of offset oscillator noise in a DMTD is imperfect.
>> The isolation amps are common base buffers. Not much gain, but quite a bit 
>> of isolation. Phase shift / C - need to look into that.
>>   
> You can achieve similar isolation together with lower noise and distortion 
> with a transformer feedback CE stage.
> Transformer feedback CB stages have even lower noise coupled with low 
> isolation, however they can be useful for amplifying low level signals ahead 
> of a high isolation amplifier.
>> 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.
>> 
>>   
> That's one of the worst terminations possible from the noise perspective.
> To lower the noise its essential to reflect the sum frequency back into the 
> mixer.
> Resistors in series with the mixer LO and RF inputs will then be required to 
> improve the mixer input VSWR.
>> 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.
>> 
>>   
> You can take the published phase noise for unspecified mixers as a lower 
> limit.
> The noise in the flicker region for the mixers (eg those from minicircuits) 
> that use integrated diode quads may be somewhat higher.
> Initial measurements on a HP10534B (uses discrete diodes) appear consistent 
> with the typical noise specs for a low level mixer.
>> 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.
>> 
>>   
> NIST's measurements indicate that lowest delay tempco is achieved with a 
> powdered silica dielectric.
> Specialised fibres can have very low delay tempcos.
>> Crazy Stuff ....
>> 
>> So what did I miss that time?
>> 
>> Bob
>> 
>>   
> Bruce
>> 
>> 
>> 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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>>>     
>> 
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> 
> 
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