[time-nuts] HP 5065A performance vs. others
Magnus Danielson
magnus at rubidium.dyndns.org
Mon Mar 22 00:21:54 UTC 2010
John Miles wrote:
>> -----Original Message-----
>> From: time-nuts-bounces at febo.com [mailto:time-nuts-bounces at febo.com]On
>> Behalf Of Bob Voelker
>> Sent: Sunday, March 21, 2010 1:59 PM
>> To: time-nuts at febo.com
>> Subject: [time-nuts] HP 5065A performance vs. others
>>
>>
>> As several postings have indicated, the performance of the HP
>> 5065A is better
>> than many of the other rubidium standards. What enables the HP 5065A to
>> achieve better performance?--Is it the physics package or the particular
>> control system implemented in electronics? Would it be possible to
>> achieve the HP 5065A's performance by modifying a more commonly
>> available rubidium such as the LPRO? Would an ensemble of LPROs
>> match a single HP 5065A in performance?
>>
>> Bob
>>
>
>
> I think those are all open questions, because it's not immediately clear
> what limits the performance of the smaller telecom-grade physics packages,
> or what low-hanging fruit might be left on the tree.
>
> For instance, how important is the length of the path the light takes
> through the filter cell and/or resonance cell? It's obviously a lot longer
> in a 5065A.
I think you would find this article of interest:
http://tycho.usno.navy.mil/ptti/1990/Vol%2022_39.pdf
Especially page 446-447.
Another mentioning of optical path length is here:
http://ntrs.nasa.gov/archive/nasa/casi.ntrs.nasa.gov/19830027087_1983027087.pdf
This Litton contribution goes into more detail about ligth-shift and
path length:
http://tycho.usno.navy.mil/ptti/1983/Vol%2015_34.pdf
Read the Ligth shift chapter starting at page 679, then check figure 4.
These is more if you care to search for Rubidium and light shift.
There is considerable amount of efforts spent on reducing light shift.
It has many sources, including lamp temperature, filter cell
temperature, filter cell length etc. etc. Filter cell
temperature-stability is a key issue from what I understand.
> the difference? Is there something special about HP's lamp? Is their microwave synthesizer that much better?
>
Could be part of it.
> HP's temperature stabilization is better than the LPro's -- so maybe it
> would help if you just moved the LPro's Rb assembly into an outer oven,
> separate from the rest of the electronics.
Temperature stability is a key issue as it connects via filter cell
light shift, lamp intensity (which spectrally needs to match that of the
filter cell... they do not match very well actually and the filter is a
bit steep), then buffert gas frequency pulling alongside of the
wall-shift. Then toss in the cavity detuning and the frequency pulling
effect that it causes.
> How important is all that
> mu-metal shielding on the 5065A, given that most people these days would
> care more about stability than absolute accuracy (thanks to GPS)?
>
The uniformity of the C-field is an issue, and if it is allowed to
change (due to externally shifting fields) well...
> Someone with more free time should tackle these questions. :) F. G. Major's
> book would be a good starting point, and this paper on laser-pumped Rb
> clocks also has a lot of hints about what limits the performance of ordinary
> sources: http://tf.nist.gov/general/pdf/1219.pdf . They used the cell from
> a commercial Rb standard in their experiment, although they didn't say which
> one. If nothing else, you can infer from this paper that the path length
> through the resonance cell isn't a huge deal.
>
Depends on how it balance with other things. See above links.
Cheers,
Magnus
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