simulating vibrational spectra in the solid state, help me!
Florian Schiffmann
flosch... at gmail.com
Mon May 13 09:21:48 UTC 2013
Hi,
as always, the answer to your question and providing help is much easier
(and likely to happen) if input files are provided.
Cp2k is a bit special for vibrational spectra. The imaginary frequencies
are not necessarily connected to a badly converged geometry. Using GTH
pseudopotentials the density at the core decays to 0. This is a bit
problematic in the xc potentials as it leads to very sharp features. These
features can cause trouble in the FFT's (see Quickstep paper, smoothing).
Cutting a long story short, if you use the GTH pseudos (and an insufficient
CUTOFF) as they are this problem leads to a slight translational invariance
of the system as the result of the FFT depends on the relative position of
the atom with respect to the grid. This problem is most obvious for 1st row
transition metals and the elements B to Na. Also it depends on the
functional as the pseudos have different parameters (BLYP pseudos are worst
from my experience). I attach a graph with some PBE test on this behaviour
and cutoffs needed to achieve a good translational invariance (<1E-5 Ha).
Keep in mind using different functionals the necessary cutoffs can be
different.
At the moment there are two ways out either you have to use a hugh cutoff
(600+ depending on your elements) or using NLCC pseudos (
http://arxiv.org/abs/1212.6011 ). The NLCC's are not yet in svn as they are
not 100% tested with every feature (energies and derivs are fine) and they
only exist for PBE and a limited number of elements (B - Cl). If you are
intersted in trying them I can send you the CP2K format. I will add them to
svn soon after testing is complete.
regards
Flo
Re
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