Re: [time-nuts] Sources for Mission Time Clock

2015-01-14 Thread Tom Van Baak
 I know precisely what you are saying and I get the feel. Nixie clocks seem
 so much cooler than seven-segment LED clocks. (And vacuum fluorescent just
 seems cheesy. Go figure.) So early '60s is retro but late '60s is not. From
 my view 50 years down the road that seems just ... humorous.

Brian, and other time nuts,

And if you don't get enough retro here, note there is an very fine Nixie 
mailing list at:
https://groups.google.com/d/forum/neonixie-L

If I had started it, it would have been called nixie-nuts ;-)

/tvb
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Re: [time-nuts] Current state of optical clocks and the definition of the second

2015-01-14 Thread Mike Feher
At those low levels, how does one differentiate between phase or AM noise? 
Thanks  Regards - Mike 

Mike B. Feher, EOZ Inc.
89 Arnold Blvd.
Howell, NJ, 07731
732-886-5960 office
908-902-3831 cell

-Original Message-
From: time-nuts [mailto:time-nuts-boun...@febo.com] On Behalf Of Bruce Griffiths
Sent: Wednesday, January 14, 2015 1:22 AM
To: Discussion of precise time and frequency measurement
Subject: Re: [time-nuts] Current state of optical clocks and the definition of 
the second

Although the phase noise when using optical combs to generate Rf signals is low 
there is no mention of the am noise.

Bruce

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Re: [time-nuts] Current state of optical clocks and the definition of the second

2015-01-14 Thread paul swed
Interestingly they use regenerative dividers.
Pretty good read.
Thanks
Paul
WB8TSL

On Tue, Jan 13, 2015 at 4:49 PM, Tom Knox act...@hotmail.com wrote:

 I think the key to this concept is an optical comb filter.
 Archita Hati of the Phase Noise measurement Group at NIST has been
 researching ultra low phase noise 5MHz references using an optical
 standard and comb filter
 as well as extensive RF components to down converting to the desired
 frequency.
 In experiments I believe she has achieved phase noise better then -154db @
 1Hz offset.
 It does appear to be the future but currently is far to large and complex
 for most if any
 practical use. I believe this link is the paper by Archita Hati I referred
 addressing
 State-of-the-Art RF Signal Generation From Optical Frequency Division.
 http://tf.boulder.nist.gov/general/pdf/2646.pdf
 Enjoy;
 Thomas Knox

 Thomas Knox



  From: namic...@gmail.com
  Date: Wed, 14 Jan 2015 07:00:09 +1100
  To: time-nuts@febo.com
  CC: namic...@gmail.com
  Subject: Re: [time-nuts] Current state of optical clocks and the
 definition   of the second
 
 
  THe stability /accuracy of lasers is entirely dependent on the cavity
 length.
  Materials used are usually invar or silica, so you are no better off than
  with a quartz crystals.
  They are just a resonant cavity.
  cheers,
  Neville Michie
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Re: [time-nuts] New algorithm, better ADEV

2015-01-14 Thread Bob Camp
Hi

Ok, now that’s looking a lot more like a counter and the normal counter 
residuals. The slope isn’t quite 1/tau, but it’s pretty close to that. Very 
nice. 

One question:

One side of the counter is running on the FE5650. What is the other side of the 
counter running on? Are the reference and input the same in this case?

Bob
 
 On Jan 14, 2015, at 10:55 AM, Li Ang lll...@gmail.com wrote:
 
 Hi
Just now, I changed the way to calculate frequency and get a better
 ADEV chart.
 http://www.qsl.net/b/bi7lnq/freqcntv4/test/20150114/0114.gif
 http://www.qsl.net/b/bi7lnq/freqcntv4/test/20150114/newway.tim
 http://www.qsl.net/b/bi7lnq/freqcntv4/test/20150114/oldway.tim
 
 
Thanks to John Miles's reply in the thread about ADEV.
 
 If you feed in frequency samples, it will convert them to phase-difference 
 samples internally, so the
 program itself doesn't really care.  The use of frequency data has a few 
 drawbacks such as less accurate
 ADEV plots due to the counter's dead time between readings, but it's the 
 easiest way to get started and is
 perfectly usable for many purposes.
 
 
 Old way:
 //reset counter every second to avoid the overflow issue
 while (1) {
 reset_fpga_counter();
 trigger_and_read_cnt(refA, sigA);
 delay_1s();
 trigger_and_read_cnt(refB, sigB);
 Freq = Calc_freq(refB - refA, sigB - sigA);
 }
 
 
 New way:
 //The counter keeps running. The software takes care of the overflow issue.
 No dead time.
 trigger_and_read_cnt(ref_prev, sig_prev);
 while (1) {
   delay_1s();
   trigger_and_read_cnt(ref_curr, sig_curr);
   ref_delta = (ref_curr  ref_prev) ? (ref_curr - ref_prev) : (0x
 - ref_prev + ref_curr);
   sig_delta = (sig_curr  sig_prev) ? (sig_curr - sig_prev) : (0x
 - sig_prev + sig_curr);
 
   Freq = CalcFreq(ref_delta, sig_delta);
   ref_prev = ref_curr;
   sig_prev = sig_curr;
 }
 
 
 BTW: I've put the counter into a box.
 http://www.qsl.net/b/bi7lnq/freqcntv4/pic/20150114_212857.jpg
 more pictures: http://www.qsl.net/b/bi7lnq/freqcntv4/pic/
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Re: [time-nuts] Current state of optical clocks and the definition of the second

2015-01-14 Thread Bob Camp
Hi

More or less by definition:

AM noise has the sidebands in phase, PM noise has the sidebands out of phase. 
PM adds to no envelope power, AM adds to the envelope power. If you have purely 
random noise, half of the power is AM, half is PM by this approach. If you have 
what is effectively a SDR (high speed ADC(s), decimators, cross correlation …) 
doing your phase noise measurement, figuring out sidebands and phase is part of 
the process. With an old style single mixer approach, you switch your operating 
point on the mixer.

Bob

 On Jan 14, 2015, at 2:19 PM, Mike Feher mfe...@eozinc.com wrote:
 
 At those low levels, how does one differentiate between phase or AM noise? 
 Thanks  Regards - Mike 
 
 Mike B. Feher, EOZ Inc.
 89 Arnold Blvd.
 Howell, NJ, 07731
 732-886-5960 office
 908-902-3831 cell
 
 -Original Message-
 From: time-nuts [mailto:time-nuts-boun...@febo.com] On Behalf Of Bruce 
 Griffiths
 Sent: Wednesday, January 14, 2015 1:22 AM
 To: Discussion of precise time and frequency measurement
 Subject: Re: [time-nuts] Current state of optical clocks and the definition 
 of the second
 
 Although the phase noise when using optical combs to generate Rf signals is 
 low there is no mention of the am noise.
 
 Bruce
 
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Re: [time-nuts] L1 and L2 frequencies

2015-01-14 Thread Brooke Clarke

Hi Martyn:

On each frequency there are a couple or more different codes.
The Civilian Acess (C/A) code on the L1 frequency is all public information and 
so is the most commonly used.

But there are classified codes that have a much higher bit rate and allow for more accurate position, time and velocity 
measurements.


Tom mentioned that there are civilian GPS receivers that make use of the L2 frequency, but they do that my using what's 
called carrier phase (that's to say they do not make use of the classified code).  This is mainly used in surveying 
applications where, by recording a lot of data and post processing, you can get a very precise location.


When two frequencies are used there's a possibility of removing an error related to the total electron count in the path 
of the signal.  The new F5 frequency allows for doing that, but as far as I know none of the commercial GPS receivers 
make use of it yet.


http://www.prc68.com/I/DAGR.shtml#GPSs

Mail_Attachment --
Have Fun,

Brooke Clarke
http://www.PRC68.com
http://www.end2partygovernment.com/2012Issues.html
http://www.prc68.com/I/DietNutrition.html
Martyn Smith wrote:

Hello,

I have some questions on GPS and GNSS.

Do all the civilian GPS receivers only operate on the L1 frequency?

Are there any GPS frequency standards out there that use L1 and L2 and that can 
be purchased by non-military customers?

I am playing with the new Lea-M8T receiver.

How do I know what satellites are GPS, GLONASS, Galileo etc.

From my understanding GLONASS have different SV numbers but not 100% sure.

Any help appreciated.

Regards

Martyn
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Re: [time-nuts] New algorithm, better ADEV

2015-01-14 Thread John Miles
 Just now, I changed the way to calculate frequency and get a better
ADEV chart.
http://www.qsl.net/b/bi7lnq/freqcntv4/test/20150114/0114.gif

Looking good!  Nice example of a white PM noise floor, just like a 'real' HP 
counter.   Let it run for a few days and see how the environmental sensitivity 
looks.

 BTW: I've put the counter into a box.
 http://www.qsl.net/b/bi7lnq/freqcntv4/pic/20150114_212857.jpg
 more pictures: http://www.qsl.net/b/bi7lnq/freqcntv4/pic/

Those small SPI LCDs are really neat, especially for the price.  I just used 
one the other day to replace a 1 CRT in a receiver panadaptor.

-- john, KE5FX
Miles Design LLC


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[time-nuts] New algorithm, better ADEV

2015-01-14 Thread Li Ang
Hi
Just now, I changed the way to calculate frequency and get a better
ADEV chart.
http://www.qsl.net/b/bi7lnq/freqcntv4/test/20150114/0114.gif
http://www.qsl.net/b/bi7lnq/freqcntv4/test/20150114/newway.tim
http://www.qsl.net/b/bi7lnq/freqcntv4/test/20150114/oldway.tim


Thanks to John Miles's reply in the thread about ADEV.

 If you feed in frequency samples, it will convert them to phase-difference 
 samples internally, so the
 program itself doesn't really care.  The use of frequency data has a few 
 drawbacks such as less accurate
 ADEV plots due to the counter's dead time between readings, but it's the 
 easiest way to get started and is
 perfectly usable for many purposes.


Old way:
//reset counter every second to avoid the overflow issue
while (1) {
 reset_fpga_counter();
 trigger_and_read_cnt(refA, sigA);
 delay_1s();
 trigger_and_read_cnt(refB, sigB);
 Freq = Calc_freq(refB - refA, sigB - sigA);
}


New way:
//The counter keeps running. The software takes care of the overflow issue.
No dead time.
trigger_and_read_cnt(ref_prev, sig_prev);
while (1) {
   delay_1s();
   trigger_and_read_cnt(ref_curr, sig_curr);
   ref_delta = (ref_curr  ref_prev) ? (ref_curr - ref_prev) : (0x
- ref_prev + ref_curr);
   sig_delta = (sig_curr  sig_prev) ? (sig_curr - sig_prev) : (0x
- sig_prev + sig_curr);

   Freq = CalcFreq(ref_delta, sig_delta);
   ref_prev = ref_curr;
   sig_prev = sig_curr;
}


BTW: I've put the counter into a box.
http://www.qsl.net/b/bi7lnq/freqcntv4/pic/20150114_212857.jpg
more pictures: http://www.qsl.net/b/bi7lnq/freqcntv4/pic/
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Re: [time-nuts] L1 and L2 frequencies

2015-01-14 Thread Martyn Smith

Hello,

I have some questions on GPS and GNSS.

Do all the civilian GPS receivers only operate on the L1 frequency?

Are there any GPS frequency standards out there that use L1 and L2 and that can 
be purchased by non-military customers?

I am playing with the new Lea-M8T receiver.

How do I know what satellites are GPS, GLONASS, Galileo etc.

From my understanding GLONASS have different SV numbers but not 100% sure.

Any help appreciated.

Regards

Martyn
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Re: [time-nuts] L1 and L2 frequencies

2015-01-14 Thread Tom Van Baak
 I have some questions on GPS and GNSS.

Note GNSS is the generic word for any satellite based navigation system. GPS is 
one of GNSS so you don't actually need to say GPS *and* GNSS.

 Do all the civilian GPS receivers only operate on the L1 frequency?

No. All the cheap ones do, though.

 Are there any GPS frequency standards out there that use L1 and L2 and that 
 can be purchased by non-military customers?

Yes. Almost all high-end survey receivers are L1 and L2. Check the web. There 
are hundreds to choose from.

 I am playing with the new Lea-M8T receiver.
 
 How do I know what satellites are GPS, GLONASS, Galileo etc.

See appendix B Satellite Numbering of your u-blox M8 Receiver Description 
manual.

 From my understanding GLONASS have different SV numbers but not 100% sure.

Each GNSS system has its own internal numbering scheme, but a multi-GNSS 
receiver has to disambiguate among them with their own scheme. Again, see the 
wonderful table on page 272.

 Any help appreciated.
 
 Regards
 
 Martyn

/tvb
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Re: [time-nuts] New algorithm, better ADEV

2015-01-14 Thread Tom Van Baak
Hi Li Ang,

You're making good progress. Thanks for the update and the photos. I am 
impressed with both the project and the way you are documenting and sharing the 
progress on the qsl.net web site.

The new algorithm is good. Yes, the whole idea of a timestamping counter is 
that you start it once and then let it run indefinitely, checking on the deltas 
only as much as you need to prevent counter aliasing.

One correction -- when you compute deltas using two's compliment integer 
variables there is no need for a special-case overflow check. This is a common 
misunderstanding by non-assembly programmers.

So, instead of your:
  ref_delta = (ref_curr  ref_prev) ? (ref_curr - ref_prev) : (0x - 
ref_prev + ref_curr);
  sig_delta = (sig_curr  sig_prev) ? (sig_curr - sig_prev) : (0x - 
sig_prev + sig_curr);

Just use:
  ref_delta = ref_curr - ref_prev;
  sig_delta = sig_curr - sig_prev;

Not only is it much simpler but it also works in every case (your code would 
fail whenever curr equals prev).

Here's a test program in case you don't believe me: 
http://leapsecond.com/tools/wrap1.c

/tvb
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Re: [time-nuts] question Alan deviation measured with Timelab and counters

2015-01-14 Thread Stéphane Rey
Bonjour Magnus,

Many thanks for your very long and detailed answer. I've read quickly bu will 
go deeper tonight.

Here are the results of today experiments... which are not giving anything 
valuable... I still don't understand the results I get  :-/

With the PM6654C, I've put the HP GPSDO on the standard input, the 1 PPS on 
channel A and the 10 MHz from the DUT (GPSDO as well) on channel B. This gives 
something in the range of 2E-9 which looks like the counter resolution, right ? 
The gating takes 4s and the Time A-B displays a value like 64 E-6
Now if I downmix the channel B to 5 kHz (LO is a DDS Standford  Reseach 
generator), I have a sinus with lower amplitude and no squarer in my hand at 
the moment to shape the signal. Anyway, I do the same operation and I get on 
the display two more digits like xx.xx E-6 but the ADEC is in the range of 
E-7 I do not understand at all this fact. Even if the slew rate is not 
great, I was expecting an improvement.
Note that the values displayed are always changing quite a lot between two 
samples. For instance with the 5 KHz channel B signal, I can read first sample 
at 27.11E-6, in the next one is 31.22E-6... which sounds huge, right ?

I've then found an HP5370A and tried the same operation. Unfortunately the 5 
kHz output is too low for the HP5370A sensitivity. I need an amplifier or 
sqauerer here but had no time to build on today.
Si I could not get anything valuable with the HP5370A at the moment...

Stephane



-Message d'origine-
De : time-nuts [mailto:time-nuts-boun...@febo.com] De la part de Magnus 
Danielson
Envoyé : mercredi 14 janvier 2015 08:04
À : time-nuts@febo.com
Cc : mag...@rubidium.se
Objet : Re: [time-nuts] question Alan deviation measured with Timelab and 
counters

Bonjour Stéphane,

On 01/14/2015 02:16 AM, Stéphane Rey wrote:
 Hi Magnus,

 For some reason I've missed this message and the one from Jim until now ! 
 This answers many of the questions I had. For my defense, I've 3000 messages 
 since the last 3 months on the list !!!

 ah, yes, I'd like to get even better than 1E-12. 1E-14 would be perfect but 
 my best standards for now are a HP GPSDO and an Effratrom FRK Rb which both 
 are around 1E-12 'only'. I may have to invest in something better if prices 
 are acceptable. I guess I won't be able to measure beyond the standard itself.

 The method you describes gives tau=2E-9 ? This is more or less what I could 
 get with the frequency measurement (even a bit lower). So what is the benefit 
 of the time interval measurement here against the frequency measurement ?

I've been sloppy with the scaling factor, so there is a fixed scaling factor 
for the noise that the single-shot resolution produces, and that would be a 
measurement limit that if everything else is ideal would dominate. This 
quantization noise is sqrt(1/12) or about 0.289 if I remember correctly, so 
that is the scale-factor. It will also have a 1/tau slope. So that is how you 
can expect this noise to behave, it will look like white phase noise, but 
isn't, it is highly systematic noise, and if you play nicely with it, you can 
measure below it. However, doing so is non-trivial.

I have one counter that does that. The good old HP5328A with the Option 
040-series of boards will introduce noise to the counting 100 MHz oscillator 
such that averaging gets you down towards 10 ps rather than
10 ns resolution in TI mode. However, it does not help you to get nice 
frequency or stability measures.

I've not taken the time to detail-analyse the ADEV scaling factor thought, I 
should do that, but it follows the general formula of
ADEV(tau) = k*t_res/tau
where t_res is the single-shot resolution and k is a constant.
There is more to this, as counters can show up non-linearities of several 
sorts, and that the trigger conditions of the input has been optimized, which 
can be slew-rate limited for many counters and conditions.

So, anyway, there is a bit of hand-waving in there, but I thought it was better 
to get you to get the basic trend there first, and then we can discuss the 
detailed numbers, as theory is one thing and achieved number can be quite a 
different one.

As for frequency and time-interval measurements, if properly done, they can be 
used interchangeably without much impact. Realize that frequency and 
time-interval measurements will both be based on time-interval measurements as 
the core observation inside the counter, so the single-shot resolution limit 
applies to them both. However, subtle details lies in how the counter works and 
there is ways that the frequency precision can be lost. A good counter is the 
SR620, but the way it does the frequency measure, you need to calibrate the 
internal delay to make it on the mark measure. Using it in time-interval mode 
and you can eliminate that offset, because the start and stop measure of your 
signal under test is done with the same channel, with essentially the same 
delay both trigger-times.


Re: [time-nuts] Sources for Mission Time Clock

2015-01-14 Thread Brian Lloyd
On Sun, Jan 11, 2015 at 10:10 PM, Wayne Holder wayne.hol...@gmail.com
wrote:


 But, 7 segment just doesn't quite capture that retro feel, IMO.


I know precisely what you are saying and I get the feel. Nixie clocks seem
so much cooler than seven-segment LED clocks. (And vacuum fluorescent just
seems cheesy. Go figure.) So early '60s is retro but late '60s is not. From
my view 50 years down the road that seems just ... humorous.

Seems like a BBB driving a good-sized 1080P display (both are cheap) would
be a good platform to do something like this. You can make it count or
display anything you want. Since the linux distro in the BBB has NTP
installed already, it should be able to keep reasonably accurate time from
a human PoV.

Hmm, I am going to want a display like that for my video wall.

-- 



Brian Lloyd
706 Flightline Drive
Spring Branch, TX 78070
br...@lloyd.aero
+1.210.802-8FLY (1.210.802-8359)
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Re: [time-nuts] question Alan deviation measured with Timelab and counters

2015-01-14 Thread Stéphane Rey
Hi John,

I hadn't noticed before you were here as well   ;-)

Thanks for answering. So I do understand I can use Timelab in frequency 
difference even if my counter sends data in TI in nanoseconds. Great.
Ah and thanks for the manual link. I didn't remember this was in the manual of 
the Timepod 
Will investigate further today

-Message d'origine-
De : time-nuts [mailto:time-nuts-boun...@febo.com] De la part de John Miles
Envoyé : mercredi 14 janvier 2015 07:26
À : 'Discussion of precise time and frequency measurement'
Objet : Re: [time-nuts] question Alan deviation measured with Timelab and 
counters

 - Can I use Frequency difference mode from Timelab to monitor time intervals ?
 If no is there a way to use the time interval measurement from the 
 counter with Timelab to plot ADEV ?

If you feed in frequency samples, it will convert them to phase-difference 
samples internally, so the program itself doesn't really care.  The use of 
frequency data has a few drawbacks such as less accurate ADEV plots due to the 
counter's dead time between readings, but it's the easiest way to get started 
and is perfectly usable for many purposes.

In general you should avoid letting the counter do any averaging.  Except in 
very specific circumstances, any apparent improvement in ADEV measurement floor 
will be illusory.   There are exceptions, but this isn't something you want to 
mess with until you're very comfortable with the rest of the measurement 
process.  Your counter's true ADEV measurement floor at t=1s should be assumed 
to be close to its single-shot resolution specification (e.g., 100 ps = about 
1E-10).

 - In case the principle of plotting ADEV from Time Interval, what is 
 the interpretation of the result ? The ADEV shows the relative 
 stability between the two GPSDO... So, practically what does it bring 
 ? And how to use this method if I want to characterize a device ?

An ADEV graph shows frequency stability statistics at different intervals, 
ranging from the rate at which the readings are returned from the counter (tau 
zero, at the left end of the plot) to a maximum interval that's related to how 
long you let the measurement run.  It's much too deep a subject to go into in 
an email; see http://www.ke5fx.com/stability.htm for more pointers.

Again, TimeLab always plots ADEV from time interval/phase data, even if you 
give it frequency readings.  ADEV is fundamentally a frequency stability 
metric, but it can be computed identically from either TI or frequency samples 
(assuming zero dead time).  
 
 - stupid question on Timelab. If I let Timelab in Auto to select the 
 period between two samples (correctly detected), the time scale of the graph 
 is wrong.
 For instance, a 3h plot stops at 2000s (0.5h)... Here again, I miss 
 something but what ?

The TimeLab manual, for one thing. :)  Hit the books (specifically 
http://www.miles.io/TimePod_5330A_user_manual.pdf , page 31).

-- john, KE5FX
Miles Design LLC


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---
L'absence de virus dans ce courrier électronique a été vérifiée par le logiciel 
antivirus Avast.
http://www.avast.com

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Re: [time-nuts] Current state of optical clocks and the definition of the second

2015-01-14 Thread Magnus Danielson



On 01/13/2015 11:41 AM, Attila Kinali wrote:

On Mon, 12 Jan 2015 20:09:45 +
Gregory Maxwell gmaxw...@gmail.com wrote:


On Mon, Jan 12, 2015 at 12:34 PM, Attila Kinali att...@kinali.ch wrote:
Seems that the state of the art in stabilized lasers has improved a
lot lately, e.g. there are commercial available 1550nm devices which
have a =3Hz line-width: http://stablelasers.com/products.html (well
on a short term basis, the medium term performance is not so
impressive)


Laser stabilization, especially for quantum metrology is still
an actively researched field. Current state of the art is IIRC
0.3Hz linewidth (sorry, cannot find the reference at the moment).
Mid- and long term stability depends highly on the reference
used. Current research is fucused mainly on special, low vibration
structures made out of low expansion glass or silicon. And these
cavities are usually put into a temperature controlled chamber in
vacuum.


Well, guess what I found standing around in a lab with an optical comb? :)

With optical line-widths in sub-Hz range and optical combs you have a 
nice way of comparing the frequency of that free-running and 
un-steerable but stable oscillator. However, as you mix it down the 
noise of the optical comb will dominate, but you can know which multiple 
of the optical comb and offset it is.



Considering the rarity and extreme cost of H-masers, or just really
exceptional quarts oscillators; might it be the case that optical LOs
start looking interesting for applications which just need stability
(or being steered by other sources; e.g. GPSDL)?


Well, an 8607 costs more than a Rb-standard. Yes, the 8607 has lower
close in phase noise and up to several 1000s it rivals the Rb, but
handling it is much more difficult than handling an Rb.
Also, if you want to buy one of those exceptionally low noise/high stable
8607's (those that go down into the 10^-14 range) you'd have to sell your car.

But, if you buy a H-maser from SpectraTime, you get a 8607 for free ;-)


That is also the only way to get the 8607 now, as Oscilloquartz is 
closing down that business.



There used to be quite some literature on how to build low noise
quartz oscillators. Most of those books are out of print today.
With two notable exceptions:

Discrete Oscillator Design: Linear, Nonlinear, Transient, and Noise Domains
by Randall Rhea, 2010

and

Understanding Quartz Crystals and Oscillators, by Ramon Cerda, 2014

I had a look at the book by Rhea, it looks quite well written and contains
a lot of real world information, but is a bit weak on the more theoretical
part (description of oscillation, noise sources,...) and thus on the
on the why things are done that way.
I didn't had the chance to buy Cerdas book yet.


An interesting book in that context is Enrico Rubiolas book on 
phase-noise, which among other things goes into explain the Leeson model 
of oscillators and it's real life design aspects.



The UFFC has some of the older books online. You need to be registered
to access them, though.

There is also a lot of knowledge on quartz crystalls hidden in old papers,
but going trough them is some serious work.

On the topic of opto-electronic oscillators, those are technologically
nice, but they are rather bulky. That's why they are mostly used in
research projects for atomic clocks. Also getting them to do low phase
noise is not that easy, and unlike quartz oscillators, there is not
much literature about that.


It's a serious bulk of glas in there, but the laser-technology as well 
as temperature-stabilization of it isn't rocket science,



(They can be down-converted to microwave frequencies using an optical
comb; a mode-locked laser whos pulses are phase locked to an incoming
beam.)


That is actually the current trend. There was a paper by NIST last year
on downconverting the beat frequency of an optical comb down to RF using
a frequency divider chain. They managed to get noise measures that rival
that of a good quartz oscillator at 5MHz. Ie at higher frequencies, it is
actually better than what a quartz oscillator can deliver.
(for some reason i have not archived that paper and google fails me)


The NIST TF archive is where you should go. Nice folks doing that work.


Certainly just the local oscillator is _closer_ to something a
time-nut might experiment with than a complete optical atomic standard
(if still not quite in reach).


Well, building a CPT based Rb vapor cell frequency standard should be feasible.
Yes, it's not a primary standard, but should do the job for most :-)

 From what i've read, using one of the MOT cells like those of
Sachser Laser [1] one might even be able to build a primary standard.
But my understanding of MOT is relatively weak and i cannot say how
difficult it actually would be. But it would be definitly a fun project
to try :-)


Building a MOT setup is relatively easy know, I have not yet seen it go 
sub 100.000 USD, but it seems like modern setups could do that if you 
let it. 

Re: [time-nuts] Current state of optical clocks and the definition of the second

2015-01-14 Thread Bruce Griffiths
Although the phase noise when using optical combs to generate Rf signals 
is low there is no mention of the am noise.

Bruce

On Tuesday, January 13, 2015 02:49:33 PM Tom Knox wrote:
 I think the key to this concept is an optical comb filter.
 Archita Hati of the Phase Noise measurement Group at NIST has been
 researching ultra low phase noise 5MHz references using an optical 
standard
 and comb filter as well as extensive RF components to down converting 
to
 the desired frequency. In experiments I believe she has achieved phase
 noise better then -154db @ 1Hz offset. It does appear to be the future 
but
 currently is far to large and complex for most if any practical use. I
 believe this link is the paper by Archita Hati I referred addressing
 State-of-the-Art RF Signal Generation From Optical Frequency Division.
 http://tf.boulder.nist.gov/general/pdf/2646.pdf
 Enjoy;
 Thomas Knox
 
 Thomas Knox
 
  From: namic...@gmail.com
  Date: Wed, 14 Jan 2015 07:00:09 +1100
  To: time-nuts@febo.com
  CC: namic...@gmail.com
  Subject: Re: [time-nuts] Current state of optical clocks and the
  definition  of the second
  
  
  THe stability /accuracy of lasers is entirely dependent on the cavity
  length. Materials used are usually invar or silica, so you are no better
  off than with a quartz crystals.
  They are just a resonant cavity.
  cheers,
  Neville Michie
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Re: [time-nuts] Current state of optical clocks and the definition of the second

2015-01-14 Thread Dr. David Kirkby (Kirkby Microwave Ltd)
Dr David Kirkby
Managing Director
Kirkby Microwave Ltd
Registered office: Stokes Hall Lodge, Burnham Rd, Chelmsford, Essex, CM3
6DT, United Kingdom
Registered in England and Wales as company number 08914892
http://www.kirkbymicrowave.co.uk/
Tel 07910 441670 / +44 7910 441670 (0900-2100 GMT)
On 13 Jan 2015 20:39, Neville Michie namic...@gmail.com wrote:
 THe stability /accuracy of lasers is entirely dependent on the cavity
length.
 Materials used are usually invar or silica, so you are no better off than
 with a quartz crystals.
 They are just a resonant cavity.
 cheers,
 Neville Michie

I do realise that thermal stability is important.  The pulsed titanium
sapphire laser I used during my PhD took about 8 hours to become stable,
and that had a lump of invar in it which was probably about 1.2 m long and
120 mm in diameter.  But to say that the stability/accuracy depends
entirely on the cavity length is a gross simplification.  Someone posted a
link to some information on getting  narrow linewidths from cheap
semiconductor lasers with something as simple as a piece of glass in front.
That does nothing to stabilise the cavity length.

There's a free webiminar on the 29th Jan at 1300 PST with the title Laser
Test of RIN, Linewidth and Optical Noise Parameters.

http://www.microwavejournal.com/events/1310-laser-test-of-rin-linewidth-and-optical-noise-parameters

Dave.
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[time-nuts] Lucent KS-24361/Z3810A : problem with Z3812A/REF 0 unit power up--RESOLVED!

2015-01-14 Thread Stan
Hello all,

 

I contacted the eBay seller and he sent me an exchange REF 0 module. I
swapped it in and it powered right up. Now there is a single green LED (ON)
illuminated on the REF 0 module and a single yellow led (STBY) illuminated
on the REF 1 module, so I'm pretty sure that all is well.

 

Thanks to everyone on this list for all of the helpful suggestions. I also
want to give the highest praise to the eBay seller, who stood behind his
product and very quickly made it right for me!

 

Regards,
Stan

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Re: [time-nuts] question Alan deviation measured with Timelab and counters

2015-01-14 Thread Magnus Danielson

Bonjour Stéphane,

On 01/14/2015 02:16 AM, Stéphane Rey wrote:

Hi Magnus,

For some reason I've missed this message and the one from Jim until now ! This 
answers many of the questions I had. For my defense, I've 3000 messages since 
the last 3 months on the list !!!

ah, yes, I'd like to get even better than 1E-12. 1E-14 would be perfect but my 
best standards for now are a HP GPSDO and an Effratrom FRK Rb which both are 
around 1E-12 'only'. I may have to invest in something better if prices are 
acceptable. I guess I won't be able to measure beyond the standard itself.

The method you describes gives tau=2E-9 ? This is more or less what I could get 
with the frequency measurement (even a bit lower). So what is the benefit of 
the time interval measurement here against the frequency measurement ?


I've been sloppy with the scaling factor, so there is a fixed scaling 
factor for the noise that the single-shot resolution produces, and that 
would be a measurement limit that if everything else is ideal would 
dominate. This quantization noise is sqrt(1/12) or about 0.289 if I 
remember correctly, so that is the scale-factor. It will also have a 
1/tau slope. So that is how you can expect this noise to behave, it will 
look like white phase noise, but isn't, it is highly systematic noise, 
and if you play nicely with it, you can measure below it. However, doing 
so is non-trivial.


I have one counter that does that. The good old HP5328A with the Option 
040-series of boards will introduce noise to the counting 100 MHz 
oscillator such that averaging gets you down towards 10 ps rather than 
10 ns resolution in TI mode. However, it does not help you to get nice 
frequency or stability measures.


I've not taken the time to detail-analyse the ADEV scaling factor 
thought, I should do that, but it follows the general formula of 
ADEV(tau) = k*t_res/tau

where t_res is the single-shot resolution and k is a constant.
There is more to this, as counters can show up non-linearities of 
several sorts, and that the trigger conditions of the input has been 
optimized, which can be slew-rate limited for many counters and conditions.


So, anyway, there is a bit of hand-waving in there, but I thought it was 
better to get you to get the basic trend there first, and then we can 
discuss the detailed numbers, as theory is one thing and achieved number 
can be quite a different one.


As for frequency and time-interval measurements, if properly done, they 
can be used interchangeably without much impact. Realize that frequency 
and time-interval measurements will both be based on time-interval 
measurements as the core observation inside the counter, so the 
single-shot resolution limit applies to them both. However, subtle 
details lies in how the counter works and there is ways that the 
frequency precision can be lost. A good counter is the SR620, but the 
way it does the frequency measure, you need to calibrate the internal 
delay to make it on the mark measure. Using it in time-interval mode 
and you can eliminate that offset, because the start and stop measure of 
your signal under test is done with the same channel, with essentially 
the same delay both trigger-times.


Another subtle detail is that when you make frequency measurements, you 
arm your counter, the start channel triggers, you wait the time you have 
programmed as the measurement time before you arm the stop channel, and 
then it triggers, after which you then read out your coarse counter of 
cycles, the interpolator states for the start and stop channels and 
well, the count of the time-base (which should be known), you calculate 
the frequency and output and well, once you cleared the bench from 
that measure you then arm the counter core of the next measurement. The 
time from the stop event to the following start event is called the 
dead-time. This dead-time is a period when the signal is not being 
observed. The actual time between the measures (time between the start 
events) and the length of the measures (time between the start and stop 
events) will not be the same, this will create a measurement bias in the 
ADEV. If you can establish the length of the dead-time you can 
compensate the measures. Very very few people do this these days, part 
of it is ignorance, part of it is why bother when you can use any of a 
number of techniques that avoid the dead-time altogether.


Being able to measure frequency does not easily convert into making 
quality ADEV measures.


Also, another danger of using frequency measures is that many modern 
counters use one of several techniques to improve the frequency 
measurement resolution by using things like linear regression. This 
behaves as a narrow-band filter, and the ADEV measures for white noise 
depend on the bandwidth of the system, and well, very very few 
measurements is annotated with their bandwidth, so traceable ADEV 
measurements will not be done there, and this pre-filtering effect 
bandwidth 

Re: [time-nuts] FOSDEM 2015 has a time-track

2015-01-14 Thread Magnus Danielson

Hi,

On 01/13/2015 11:48 AM, Attila Kinali wrote:

On Tue, 13 Jan 2015 01:57:56 -0800
Tom Van Baak t...@leapsecond.com wrote:


I was told some of the time slots of https://fosdem.org/2015/schedule/track/ 
time/
might be tentative


Well, it's FOSDEM. It's not a professionally organised conference.
And as presentations often take longer than their time slot, the schedule
tends to shift around quite a bit.


but we'll all get together after the last talk, whenever it is. So far
everyone I've heard from has the evening open.



Time nuts -- if you're within a couple hundred km of Brussels it should be 
worth it -- Sunday, 2015-02-01.


If you are new to FOSDEM, don't miss the social event on friday evening.


Who knows, Tom's beard mignt not be the only one to show up. :)

Good to know that Fridays session might be worth getting to. Thanks for 
the heads up Attila.


Cheers,
Magnus
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