Great to hear form you Alexander The mailing list is not really a lions den but you would
be forgiven for thinking so. Ok Zuev, you have mistook my meaning in your point 4.1
below. It is not supposed to be “Self-explanatory”. The unreasonable conditions
I gave for when the convolution
approach is not valid was to show how unreasonable I believe the following
is: "Reefman has shown, by analyzing the effect
of transparency, that the convolution model is not valid in the
general case." In other words of course it is “not valid in
the general case”. Either one says that something is adequate for a purpose or
inadequate for a purpose and not just simply
inadequate. Let’s not get into word games as this I am sure would
bore everyone. Now you say below that you were not critical of the
convolution approach but only guided by the opinions of the authors of the
convolution approach. It is Ok to
be critical of something if you have reason to
be . Let’s expand on the text: “It
must be emphasized that the instrumental function Ju(E)
is
an approximation. Reefman has shown, by analyzing the effect of
transparency, that the convolution model is not valid in the
general case." Thus I guess is just another author’s
opinion; enough said. I would like to comment now on your new approach which I am sure is far more interesting for you. In your approach I understand the fact that each ray is treated analytically in regards to its origin on the source, its diffraction on the sample whcih then leads to a cone. Grids however as stated are necessary for the source and the sample and of course accuracy is dependent on the number of grid points. For sample transparency the grid would need to be three dimensional ; how on earth do you propose to speed that up. Good luck with it. Also dont be surprised if you stick with that approach for axial divergence as in the Full axial model and use convolution for the lesser abberations. I look forward to seeing a fine tuned version sometime in the future. By the way I stopped using assembler at least 5 years ago as compilers today do the job. All the
best Alan Coelho
From: Zuev [mailto:[EMAIL PROTECTED] Sent: Thursday, 1 June 2006 1:24 AM To: rietveld_l@ill.fr Subject: RE: how to find out POLARISATION Factor Dear Dr. A.
Coelho, dear Rietvelders there are four points to be
considered. 1. Precision of the fit (using the
convolution approach). 2. Theoretical basis of the
convolution approach. 3. Calculation time with the method
in my paper. 4. “… some inaccuracies of the above
mentioned paper” 1. There is no doubt that
convolution approach provides good agreement in profile fitting with ray
traycing. 2. It is not obviously with the
rigorous theoretical validation of the convolution method.
I mean the following
aspects: a) Strictly speaking, even the flat
specimen aberration coupled with the receiving slit width
can not be mathematically
described as convolution. It is not critique, but just a
statement of fact. Well, the convolution can be used,
but this is only approximation
(even
if it is good for the certain conditions). b) The same is valid for the axial
aberration. Also the treatment of the axial aberration is an approximation
(“More recently Cheary and Coelho
[3,4] have developed a semi-analytical approach to the calculation and their results
have been incorporated into a profile refinement procedure.” From
R. W. Cheary, A. A. Coelho, J. P. Cline. Fundamental
Parameters Line Profile Fitting in Laboratory Diffractometers, J. Res. Natl.
Inst. Stand. Technol. 109, 1-25
(2004)) 3. Calculation time. There is only
the approach in my article was represented. It makes possible to develop a
number of the (exact) modifications and approximations (without lost
of accuracy). I had not yet made optimization.
I mean not the code optimization “at
an assembler code level” (From R. W. Cheary, A. A. Coelho, J. P. Cline. Fundamental
Parameters Line Profile Fitting in Laboratory Diffractometers, J. Res. Natl.
Inst. Stand. Technol. 109, 1-25
(2004))),
but only the mathematical
algorithms. Partly I have made it. 4. About “some inaccuracies of the
above mentioned paper” 1) The reference was made on page
310-311 and to quote the text of "Reefman has shown, by analyzing the
effect of transparency, that the convolution model is not valid in the general
case." This of course is correct as the
convolution approach is not valid for axial divergence greater than probably 10
degrees in both the primary and
secondary beams and linear absorption coefficients less than 10
(1/cm). Self-explanatory. 2) Back to the paper by about the influence of coupling
specific instrumental functions in FPA, it is also necessary to tune
the fundamental parameters to allow
a best fit for the experimental data (Cheary et al.,
2004)." Coupling effects were always
investigated during the development of FPA by Cheary and Coelho.
This led to the need to partially
number cruch the Full Axial Model which considers primary
and secondary axial divergence
together. I would like to cite the other
paper: “Fine tuning is sometimes
necessary to accommodate a monochromator or to compensate for the
fact that certain aberrations are
not completely independent [8].”
(From R. W.
Cheary, A. A. Coelho, J. P. Cline. Fundamental
Parameters Line Profile Fitting in Laboratory Diffractometers, J. Res. Natl.
Inst. Stand. Technol. 109, 1-25
(2004)) OK, it may be significant whether
the fundamental parameter are fine tuned intentionally
to compensate coupling effect, or to
compensate for lack of knowledge. I would like to emphasize that I had
not criticized the convolution approach, but I was only guided by the
opinion of the authors of the
convolution approach. With best regards, |
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