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Re: [time-nuts] hm H Maser

BG
Bruce Griffiths
Mon, Jan 9, 2017 6:05 AM

For a rubidium vpour standard a cavity is essential, one could always use a
microwave horn to illuminate the cell in an anechoic chamber.
Using an integrating sphere can enhance the contrast of the optical signal
significantly.

http://www.princeton.edu/physics/graduate-program/theses/theses-from-2011-1/bmcguyer_dissertation.pdf

https://infoscience.epfl.ch/record/178228/files/IFCS_Invited_Talk_Finalpdf.pdf

https://doc.rero.ch/record/32317/files/00002318.pdf

http://tf.nist.gov/general/pdf/1154.pdf

http://tf.boulder.nist.gov/general/pdf/1663.pdf

Bruce
On Sunday, January 08, 2017 10:20:33 PM Bruce Griffiths wrote:

Possible sources of Rubium vapour

cells:https://www.thorlabs.com/newgrouppage9.cfm?objectgroup_id=1470

http://www.precisionglassblowing.com/custom-solutions/optical-glassware/vapo
r-wavelength-reference-cells/

https://www.sacher-laser.com/home/lab-equipment/spectroscopy/reference_gas_a
nd_vapor_cells/reference_gas_and_vapor_cells.html

Bruce

 On Monday, 9 January 2017 11:14 AM, Bruce Griffiths

bruce.griffiths@xtra.co.nz wrote:

Bob
As long as one stays away from CPT and merely uses the laser as a
replacement for the traditional rubidium lamp plus filters it should be
easy enough as one doesnt need to modulate the laser at 3.4 GHz.I was
thinking something along the lines of the recent PhD thesis that gave all
the detail required to duplicate their low noise rubidium standard that

was

quieter than am HP5065.One could easily substitute ones own ECDL

(These can

easily be constructed from commercially available parts) and improve
somewhat on the performance (The oven design of most commercial

ECDLs seems

suboptimal). Bruce

 On Monday, 9 January 2017 10:23 AM, Bob Camp <kb8tq@n1k.org> 

wrote:

Hi

The large diameter Rb cells are a bit harder to come by than the more
generic telecom sized cells. I suspect you are correct and they are out
there from somebody.. The real advantage you would have with an Rb is

that

the design you do is gigantic compared to what everybody is doing

today.

Their constraints are not your constraints.

Based on the laser driven Rb on my bench …. don’t bother with that part

of

it. It is indeed doable. Doing it in a fashion that gives you a better
standard …. not really easy at all.

Bob

On Jan 8, 2017, at 3:55 PM, Bruce Griffiths

wrote:

The rubidium standard appears much more manageable given that

the cavity

dimensions are somewhat more compact and rubidium vapour cells

are

readily available. Substituting a laser for the lamp should also help in
improving the reliability. However an ECDL laser locked to a rubidium
line is required for a double resonance setup. Building ones own ECDL
doesn't appear to be particularly daunting, however low noise drive
electronics will be required. All the necessary optics are off the shelf
items. One still has the issue of  the frequency pulling due to the
presence of the vapour cell. Bruce

On Sunday, January 08, 2017 10:22:54 AM you wrote:

Hi

I guess the question then would be:

Is a H Maser that runs 6.6 x 10^-12 at 1 second worth the trouble?

With 100 KHz / C temperature coefficients running around, getting
good stability in a real world setting at 1 day will be “interesting”.

Just for reference:  The MH-2010 data sheet shows 1.5x10^-13 at
1 second for the “cheap” version and 8x10^-14 at one second for
the low noise version.  Data showing the 5065 Rb at 1x10^-12 at
1 second is running around on various web sites.

The NIST paper suggests that they made several prototypes before
they got one good one working. That’s a lot of “fun and games” with
ceramic machine lathes and Rb magnetometers…..

The punch line being - would the same effort / cost / many years of

time

be
more fruitful (ADEV wise) doing a large package Rb (like a 5065) ?
Based
on the number of people making them in volume over the years,

Rb’s

appear
to be the easier item to debug, design, and build.

Bob

On Jan 8, 2017, at 6:01 AM, Bruce Griffiths
bruce.griffiths@xtra.co.nz
wrote:

You could try a cavity like the one
in;http://tf.nist.gov/general/pdf/156.pdf

This avoids the requirement for a fused quartz storage bulb.
Bruce

On Sunday, 8 January 2017 11:33 PM, timeok 

Hi,
the thought of being able to work on building a H Maser has

always

accompanied me in recent years. I fully understand the many
difficulties
of this project and also the necessity of a work team. Maybe a

Passive

Maser would be easiest to implement, but I do not know in detail

the

processes of construction of the physical part of the

interrogation.

For a rubidium vpour standard a cavity is essential, one could always use a microwave horn to illuminate the cell in an anechoic chamber. Using an integrating sphere can enhance the contrast of the optical signal significantly. http://www.princeton.edu/physics/graduate-program/theses/theses-from-2011-1/bmcguyer_dissertation.pdf https://infoscience.epfl.ch/record/178228/files/IFCS_Invited_Talk_Finalpdf.pdf https://doc.rero.ch/record/32317/files/00002318.pdf http://tf.nist.gov/general/pdf/1154.pdf http://tf.boulder.nist.gov/general/pdf/1663.pdf Bruce On Sunday, January 08, 2017 10:20:33 PM Bruce Griffiths wrote: > Possible sources of Rubium vapour > cells:https://www.thorlabs.com/newgrouppage9.cfm?objectgroup_id=1470 > > http://www.precisionglassblowing.com/custom-solutions/optical-glassware/vapo > r-wavelength-reference-cells/ > > https://www.sacher-laser.com/home/lab-equipment/spectroscopy/reference_gas_a > nd_vapor_cells/reference_gas_and_vapor_cells.html > > > Bruce > > On Monday, 9 January 2017 11:14 AM, Bruce Griffiths > <bruce.griffiths@xtra.co.nz> wrote: > > > Bob > As long as one stays away from CPT and merely uses the laser as a > replacement for the traditional rubidium lamp plus filters it should be > easy enough as one doesnt need to modulate the laser at 3.4 GHz.I was > thinking something along the lines of the recent PhD thesis that gave all > the detail required to duplicate their low noise rubidium standard that was > quieter than am HP5065.One could easily substitute ones own ECDL (These can > easily be constructed from commercially available parts) and improve > somewhat on the performance (The oven design of most commercial ECDLs seems > suboptimal). Bruce > > On Monday, 9 January 2017 10:23 AM, Bob Camp <kb8tq@n1k.org> wrote: > > > Hi > > The large diameter Rb cells are a bit harder to come by than the more > generic telecom sized cells. I suspect you are correct and they are out > there from somebody.. The real advantage you would have with an Rb is that > the design you do is gigantic compared to what everybody is doing today. > Their constraints are not your constraints. > > Based on the laser driven Rb on my bench …. don’t bother with that part of > it. It is indeed doable. Doing it in a fashion that gives you a better > standard …. not really easy at all. > > Bob > > > On Jan 8, 2017, at 3:55 PM, Bruce Griffiths <bruce.griffiths@xtra.co.nz> > > wrote: > > > > The rubidium standard appears much more manageable given that the cavity > > dimensions are somewhat more compact and rubidium vapour cells are > > readily available. Substituting a laser for the lamp should also help in > > improving the reliability. However an ECDL laser locked to a rubidium > > line is required for a double resonance setup. Building ones own ECDL > > doesn't appear to be particularly daunting, however low noise drive > > electronics will be required. All the necessary optics are off the shelf > > items. One still has the issue of the frequency pulling due to the > > presence of the vapour cell. Bruce > > > > On Sunday, January 08, 2017 10:22:54 AM you wrote: > > > Hi > > > > > > I guess the question then would be: > > > > > > Is a H Maser that runs 6.6 x 10^-12 at 1 second worth the trouble? > > > > > > With 100 KHz / C temperature coefficients running around, getting > > > good stability in a real world setting at 1 day will be “interesting”. > > > > > > Just for reference: The MH-2010 data sheet shows 1.5x10^-13 at > > > 1 second for the “cheap” version and 8x10^-14 at one second for > > > the low noise version. Data showing the 5065 Rb at 1x10^-12 at > > > 1 second is running around on various web sites. > > > > > > The NIST paper suggests that they made several prototypes before > > > they got one good one working. That’s a lot of “fun and games” with > > > ceramic machine lathes and Rb magnetometers….. > > > > > > The punch line being - would the same effort / cost / many years of time > > > be > > > more fruitful (ADEV wise) doing a large package Rb (like a 5065) ? > > > Based > > > on the number of people making them in volume over the years, Rb’s > > > appear > > > to be the easier item to debug, design, and build. > > > > > > Bob > > > > > > > On Jan 8, 2017, at 6:01 AM, Bruce Griffiths > > > > <bruce.griffiths@xtra.co.nz> > > > > wrote: > > > > > > > > You could try a cavity like the one > > > > in;http://tf.nist.gov/general/pdf/156.pdf > > > > > > > > This avoids the requirement for a fused quartz storage bulb. > > > > Bruce > > > > > > > > On Sunday, 8 January 2017 11:33 PM, timeok <timeok@timeok.it> wrote: > > > > Hi, > > > > the thought of being able to work on building a H Maser has always > > > > accompanied me in recent years. I fully understand the many > > > > difficulties > > > > of this project and also the necessity of a work team. Maybe a Passive > > > > Maser would be easiest to implement, but I do not know in detail the > > > > processes of construction of the physical part of the interrogation.
BC
Bob Camp
Mon, Jan 9, 2017 12:56 PM

Hi

On Jan 9, 2017, at 1:05 AM, Bruce Griffiths bruce.griffiths@xtra.co.nz wrote:

For a rubidium vpour standard a cavity is essential, one could always use a
microwave horn to illuminate the cell in an anechoic chamber.

The cavity in an Rb is not the ultra high Q monster that you have in a Maser. There is
no magic “minimum Q” requirement to get the beast to work. That’s by no means saying
that the cavity is unimportant or trivial. The point is only that it’s about 2 orders of magnitude
easier to make up the required cavity for the Rb.

It should be noted that cavity != shielding and that cavity != temperature control. It is simply
the microwave resonant structure that gets the electromagnetic doing the right thing. In both
cases you still need (very) good magnetic shielding, pressure shielding, and temperature
control. In the Rb case, you need to set up specific temperatures to get things to work in
each cell. In the Maser case you simply need the “right” temperature for your setup.

Traditionally one of the big deals about both devices was the synthesizer required to convert
the physics based frequency to something useful. With the Maser the frequency is pretty
much always the same number. That gives a simpler synthesizer in terms of tuning. A whole
raft of this and that give you a range of answers for the Rb. That used to make the synthesizer
a bit of  a pain to design. These days, the synthesizer tuning the Rb requires is easily done with
a cheap DDS chip. Take a look at the 5065 manual if you want to see how much fun that
used to be …

Indeed the whole electronics side of both standards is easier than it once was. The temperature
probes in the compact Maser still are $1K each, but most of the parts you need on the electronics
side are pretty common items. Again, common parts != trivial design. You still need to get the
details right. Signal to noise does matter. You need to use the right design with the right parts.

So how do you do this? The normal approach is to get a dozen or so people together and work
on it 40 hours a week for about 5 years. You build up a series of batches of prototypes and
get to the point you believe you have a design (1 in 10 sort of works). You then spend roughly
another three to five years knocking the rough edges off of that design and making the first
batch of real units. Beyond time and people there is the cost of parts, software licenses, normal
test gear, really weird test gear, and all the other stuff.  This assumes it is run as a business with
somebody managing the whole thing. Try to run it as a committee of the whole, both the cost
and the time will go up. Try to do it without the right tools, at lest the time will go up. I’d bet
the cost will go up as well…

Bob

Possible sources of Rubium vapour

cells:https://www.thorlabs.com/newgrouppage9.cfm?objectgroup_id=1470

http://www.precisionglassblowing.com/custom-solutions/optical-glassware/vapo
r-wavelength-reference-cells/

https://www.sacher-laser.com/home/lab-equipment/spectroscopy/reference_gas_a
nd_vapor_cells/reference_gas_and_vapor_cells.html

Bruce

On Monday, 9 January 2017 11:14 AM, Bruce Griffiths

bruce.griffiths@xtra.co.nz wrote:

Bob
As long as one stays away from CPT and merely uses the laser as a
replacement for the traditional rubidium lamp plus filters it should be
easy enough as one doesnt need to modulate the laser at 3.4 GHz.I was
thinking something along the lines of the recent PhD thesis that gave all
the detail required to duplicate their low noise rubidium standard that

was

quieter than am HP5065.One could easily substitute ones own ECDL

(These can

easily be constructed from commercially available parts) and improve
somewhat on the performance (The oven design of most commercial

ECDLs seems

suboptimal). Bruce

On Monday, 9 January 2017 10:23 AM, Bob Camp <kb8tq@n1k.org> 

wrote:

Hi

The large diameter Rb cells are a bit harder to come by than the more
generic telecom sized cells. I suspect you are correct and they are out
there from somebody.. The real advantage you would have with an Rb is

that

the design you do is gigantic compared to what everybody is doing

today.

Their constraints are not your constraints.

Based on the laser driven Rb on my bench …. don’t bother with that part

of

it. It is indeed doable. Doing it in a fashion that gives you a better
standard …. not really easy at all.

Bob

On Jan 8, 2017, at 3:55 PM, Bruce Griffiths

wrote:

The rubidium standard appears much more manageable given that

the cavity

dimensions are somewhat more compact and rubidium vapour cells

are

readily available. Substituting a laser for the lamp should also help in
improving the reliability. However an ECDL laser locked to a rubidium
line is required for a double resonance setup. Building ones own ECDL
doesn't appear to be particularly daunting, however low noise drive
electronics will be required. All the necessary optics are off the shelf
items. One still has the issue of  the frequency pulling due to the
presence of the vapour cell. Bruce

On Sunday, January 08, 2017 10:22:54 AM you wrote:

Hi

I guess the question then would be:

Is a H Maser that runs 6.6 x 10^-12 at 1 second worth the trouble?

With 100 KHz / C temperature coefficients running around, getting
good stability in a real world setting at 1 day will be “interesting”.

Just for reference:  The MH-2010 data sheet shows 1.5x10^-13 at
1 second for the “cheap” version and 8x10^-14 at one second for
the low noise version.  Data showing the 5065 Rb at 1x10^-12 at
1 second is running around on various web sites.

The NIST paper suggests that they made several prototypes before
they got one good one working. That’s a lot of “fun and games” with
ceramic machine lathes and Rb magnetometers…..

The punch line being - would the same effort / cost / many years of

time

be
more fruitful (ADEV wise) doing a large package Rb (like a 5065) ?
Based
on the number of people making them in volume over the years,

Rb’s

appear
to be the easier item to debug, design, and build.

Bob

On Jan 8, 2017, at 6:01 AM, Bruce Griffiths
bruce.griffiths@xtra.co.nz
wrote:

You could try a cavity like the one
in;http://tf.nist.gov/general/pdf/156.pdf

This avoids the requirement for a fused quartz storage bulb.
Bruce

On Sunday, 8 January 2017 11:33 PM, timeok

Hi,
the thought of being able to work on building a H Maser has

always

accompanied me in recent years. I fully understand the many
difficulties
of this project and also the necessity of a work team. Maybe a

Passive

Maser would be easiest to implement, but I do not know in detail

the

processes of construction of the physical part of the

interrogation.


time-nuts mailing list -- time-nuts@febo.com
To unsubscribe, go to https://www.febo.com/cgi-bin/mailman/listinfo/time-nuts
and follow the instructions there.

Hi > On Jan 9, 2017, at 1:05 AM, Bruce Griffiths <bruce.griffiths@xtra.co.nz> wrote: > > For a rubidium vpour standard a cavity is essential, one could always use a > microwave horn to illuminate the cell in an anechoic chamber. The cavity in an Rb is not the ultra high Q monster that you have in a Maser. There is no magic “minimum Q” requirement to get the beast to work. That’s by no means saying that the cavity is unimportant or trivial. The point is only that it’s about 2 orders of magnitude easier to make up the required cavity for the Rb. It should be noted that cavity != shielding and that cavity != temperature control. It is simply the microwave resonant structure that gets the electromagnetic doing the right thing. In both cases you still need (very) good magnetic shielding, pressure shielding, and temperature control. In the Rb case, you need to set up specific temperatures to get things to work in each cell. In the Maser case you simply need the “right” temperature for your setup. Traditionally one of the big deals about both devices was the synthesizer required to convert the physics based frequency to something useful. With the Maser the frequency is pretty much always the same number. That gives a simpler synthesizer in terms of tuning. A whole raft of this and that give you a range of answers for the Rb. That used to make the synthesizer a bit of a pain to design. These days, the synthesizer tuning the Rb requires is easily done with a cheap DDS chip. Take a look at the 5065 manual if you want to see how much fun that used to be … Indeed the whole electronics side of both standards is easier than it once was. The temperature probes in the compact Maser still are $1K each, but most of the parts you need on the electronics side are pretty common items. Again, common parts != trivial design. You still need to get the details right. Signal to noise *does* matter. You need to use the right design with the right parts. So how do you do this? The normal approach is to get a dozen or so people together and work on it 40 hours a week for about 5 years. You build up a series of batches of prototypes and get to the point you believe you have a design (1 in 10 sort of works). You then spend roughly another three to five years knocking the rough edges off of that design and making the first batch of real units. Beyond time and people there is the cost of parts, software licenses, normal test gear, really weird test gear, and all the other stuff. This assumes it is run as a business with somebody managing the whole thing. Try to run it as a committee of the whole, both the cost and the time will go up. Try to do it without the right tools, at lest the time will go up. I’d bet the cost will go up as well… Bob > Using an integrating sphere can enhance the contrast of the optical signal > significantly. > > http://www.princeton.edu/physics/graduate-program/theses/theses-from-2011-1/bmcguyer_dissertation.pdf > > https://infoscience.epfl.ch/record/178228/files/IFCS_Invited_Talk_Finalpdf.pdf > > https://doc.rero.ch/record/32317/files/00002318.pdf > > http://tf.nist.gov/general/pdf/1154.pdf > > http://tf.boulder.nist.gov/general/pdf/1663.pdf > > > Bruce > On Sunday, January 08, 2017 10:20:33 PM Bruce Griffiths wrote: >> Possible sources of Rubium vapour >> > cells:https://www.thorlabs.com/newgrouppage9.cfm?objectgroup_id=1470 >> >> http://www.precisionglassblowing.com/custom-solutions/optical-glassware/vapo >> r-wavelength-reference-cells/ >> >> https://www.sacher-laser.com/home/lab-equipment/spectroscopy/reference_gas_a >> nd_vapor_cells/reference_gas_and_vapor_cells.html >> >> >> Bruce >> >> On Monday, 9 January 2017 11:14 AM, Bruce Griffiths >> <bruce.griffiths@xtra.co.nz> wrote: >> >> >> Bob >> As long as one stays away from CPT and merely uses the laser as a >> replacement for the traditional rubidium lamp plus filters it should be >> easy enough as one doesnt need to modulate the laser at 3.4 GHz.I was >> thinking something along the lines of the recent PhD thesis that gave all >> the detail required to duplicate their low noise rubidium standard that > was >> quieter than am HP5065.One could easily substitute ones own ECDL > (These can >> easily be constructed from commercially available parts) and improve >> somewhat on the performance (The oven design of most commercial > ECDLs seems >> suboptimal). Bruce >> >> On Monday, 9 January 2017 10:23 AM, Bob Camp <kb8tq@n1k.org> > wrote: >> >> >> Hi >> >> The large diameter Rb cells are a bit harder to come by than the more >> generic telecom sized cells. I suspect you are correct and they are out >> there from somebody.. The real advantage you would have with an Rb is > that >> the design you do is gigantic compared to what everybody is doing > today. >> Their constraints are not your constraints. >> >> Based on the laser driven Rb on my bench …. don’t bother with that part > of >> it. It is indeed doable. Doing it in a fashion that gives you a better >> standard …. not really easy at all. >> >> Bob >> >>> On Jan 8, 2017, at 3:55 PM, Bruce Griffiths > <bruce.griffiths@xtra.co.nz> >>> wrote: >>> >>> The rubidium standard appears much more manageable given that > the cavity >>> dimensions are somewhat more compact and rubidium vapour cells > are >>> readily available. Substituting a laser for the lamp should also help in >>> improving the reliability. However an ECDL laser locked to a rubidium >>> line is required for a double resonance setup. Building ones own ECDL >>> doesn't appear to be particularly daunting, however low noise drive >>> electronics will be required. All the necessary optics are off the shelf >>> items. One still has the issue of the frequency pulling due to the >>> presence of the vapour cell. Bruce >>> >>> On Sunday, January 08, 2017 10:22:54 AM you wrote: >>>> Hi >>>> >>>> I guess the question then would be: >>>> >>>> Is a H Maser that runs 6.6 x 10^-12 at 1 second worth the trouble? >>>> >>>> With 100 KHz / C temperature coefficients running around, getting >>>> good stability in a real world setting at 1 day will be “interesting”. >>>> >>>> Just for reference: The MH-2010 data sheet shows 1.5x10^-13 at >>>> 1 second for the “cheap” version and 8x10^-14 at one second for >>>> the low noise version. Data showing the 5065 Rb at 1x10^-12 at >>>> 1 second is running around on various web sites. >>>> >>>> The NIST paper suggests that they made several prototypes before >>>> they got one good one working. That’s a lot of “fun and games” with >>>> ceramic machine lathes and Rb magnetometers….. >>>> >>>> The punch line being - would the same effort / cost / many years of > time >>>> be >>>> more fruitful (ADEV wise) doing a large package Rb (like a 5065) ? >>>> Based >>>> on the number of people making them in volume over the years, > Rb’s >>>> appear >>>> to be the easier item to debug, design, and build. >>>> >>>> Bob >>>> >>>>> On Jan 8, 2017, at 6:01 AM, Bruce Griffiths >>>>> <bruce.griffiths@xtra.co.nz> >>>>> wrote: >>>>> >>>>> You could try a cavity like the one >>>>> in;http://tf.nist.gov/general/pdf/156.pdf >>>>> >>>>> This avoids the requirement for a fused quartz storage bulb. >>>>> Bruce >>>>> >>>>> On Sunday, 8 January 2017 11:33 PM, timeok > <timeok@timeok.it> wrote: >>>>> Hi, >>>>> the thought of being able to work on building a H Maser has > always >>>>> accompanied me in recent years. I fully understand the many >>>>> difficulties >>>>> of this project and also the necessity of a work team. Maybe a > Passive >>>>> Maser would be easiest to implement, but I do not know in detail > the >>>>> processes of construction of the physical part of the > interrogation. > _______________________________________________ > time-nuts mailing list -- time-nuts@febo.com > To unsubscribe, go to https://www.febo.com/cgi-bin/mailman/listinfo/time-nuts > and follow the instructions there.