Shay,

    I have to disagree with much of the previous discussion. Yes, there are 
aberrations in two-theta with sample displacement in a pseudo-parallel beam 
instrument and they are different for displacement along the beam direction and 
for displacement perpendicular to the beam (but in the detection plane). 
Typically you can only see the first correction when data are collected over a 
very wide angular range (>150 degrees) so this is almost never noticed with 
x-rays. The functional form for the corrections is coded into GSAS-II, so if 
you want read through the source code you can see what they are or you can do 
some simulations to see the effect. The functional form for these corrections 
are completely different from those for Bragg-Brentato geometry, which is 
extremely sensitive to the sample height and in some cases sample transparency.

   The Debye-Sherrer geometry corrections are typically very minor. When only 
the second term is needed, the correction can be replaced with small shifts in 
the two-theta zero correction and lattice constants. This is why in practice 
with synchrotrons and CW neutrons one does not see the problems with sample 
placement that leads to large peak shifts in a Bragg-Brentano geometry, making 
it much easier to index patterns from synchrotron data, but it is not true that 
there are no corrections.

Brian


On Feb 2, 2017, at 9:14 AM, Shay Tirosh 
<[email protected]<mailto:[email protected]>> wrote:

Dear Rietvelders

Does the 2-teta shift due to sample displacement in parallel beam is similar to 
Bragg Brentano mode?
If not then what is the mathematical expression in parallel beam?

Thanks

Shay
--
_________________________________________________

Dr. Shay Tirosh
Institute for Nanotechnology & Advanced Materials
Bar Ilan University
Ramat Gan, 52900
Israel
Phone: +972-(0)30-531-7320
Mobile: +972-(0)54-8834533
Email: [email protected]<mailto:[email protected]>
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