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> I believe he means something that is relevant to real life where
> crystals are small, diffraction weak, and background high, i.e. a
> quantity that can realistically be extracted from the crap we get on
our
> images.

Frank, my point was that in the presence of DS (which for protein
crystals mean always), it's actually impossible to extract the Bragg
component from the images without assuming some kind of model for the
DS, i.e. anywhere in the spectrum between the simplistic 'tails' method
(which is of course empirical and approximate), to a full-blown
dynamical model.  I believe pretty well everyone agrees that I(Bragg) is
defined as the component of the diffraction arising from the average
density, and we don't need to define it any other way.

Note that I'm *not* saying that *none* of the DS can be modelled by a
planar background: only the 'optic' & 'acoustic' contributions are
sufficiently non-uniform that a planar background model won't remove
them.  The other main contribution, named after A. Einstein after his
model of a solid as a lattice of independent quantum harmonic
oscillators, and which arises from correlated displacements of electrons
attached to atoms whose mean displacements are uncorrelated relative to
all the other atoms, is sufficiently locally uniform that it can be
modelled by a planar background, and therefore the integrated intensity
obtained consists only of I(Bragg) + I(DSacoustic) + I(DSoptic).

Cheers

-- Ian


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