Hi

A spherical set of cells is going to be a massive pain to fabricate. I believe 
you can hit < 5x10^-12 / sqrt(tau) with 
a fairly normal cell design and cavity design. There are some very basic issues 
with the photo detector’s S/N that
also tip things towards a coaxial approach.

Bob

> On Jan 10, 2017, at 10:43 PM, Bruce Griffiths <bruce.griffi...@xtra.co.nz> 
> wrote:
> 
> A  spherical cavity resonator with a spherical Rubidium cell configured as an 
> integrating sphere (to enhance the SNR of the optical absorption signal) is a 
> potential option. Its also possible to use the same cell to lock a 795 nm 
> laser to the desired wavelength. Fiber coupling the laser light could also be 
> useful.Note that with an integrating sphere (or any other random scattering 
> process eg scattering from colloidal particles undergoing Brownian motion) 
> laser polarisation isn't preserved which may be convenient.One potential 
> issue with an  integrating sphere is the longevity of the diffusing coating 
> (typically Barium sulphate with an organic binder). Roughening (fine grind  
> followed by HF etch for stress relief) the outer surface of the cell is also 
> advisable to eliminate light pipe effects in the cell wall.
> Bruce 
> 
>    On Wednesday, 11 January 2017 3:54 PM, Bruce Griffiths 
> <bruce.griffi...@xtra.co.nz> wrote:
> 
> 
> A goal with ADEV ~ 1E-13/Tau (for Tau <1000sec) may be feasible as its 
> already been done as part of a PhD thesis.Using as large a cavity as possible 
> is probably useful so that a large cell can be employed.What resonant mode is 
> desirable in the cavity?Do we need to avoid field reversal as in the hydrogen 
> maser?
> Bruce  
> 
>    On Wednesday, 11 January 2017 3:43 PM, Bob Camp <kb...@n1k.org> wrote:
> 
> 

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