CCL: AW: CASSCF does not produce spin densities



I think that this is a reasonable way to approach the problem, but it needs some generalization from the way that most physicists I know think about it.  In my experience, one is almost always referring to an underlying Fermi liquid model, in which case there are simple poles in the response function.  In the case of e.g. CAS models, it is not clear that the poles are all simple.   If state-averaged methods are also to be treated, then it would seem that the self-energy must be described using an operator formalism (i.e. an operator acting on the target space), which would complicate things.  For non-evenly weighted averages, it is not clear how to think about the weights (because the state-averaged density matrix is no longer dual to a von Neumann measurement, but instead to a POVM - a metric needs to be introduced).  -SEth

On 15/03/2012, at 6:19 PM, Georg Lefkidis lefkidis**physik.uni-kl.de wrote:


Sent to CCL by: "Georg Lefkidis" [lefkidis^^physik.uni-kl.de]
Dear Jürgen, dear all

the problem of defining static vs. dynamical correlations is not an easy
one. I have discussed it many times with my physicists colleagues and the
consensus (for whatever this is worth) is that dynamic correlations are
defined by virtual excitations with well-defined, nonzero energy
differences. Following this trail of thoughts the “measure” of the character
of the correlations is the energy difference of the Slater determinants in
the CI expansion. This is also consistent with the fact that for static
correlations one needs multi-reference expansions. This is also connected to
the self-energy, in that the static correlations stem from its imaginary
part while dynamic mainly originate from its real part.  I am not sure I
completely understand this, however. My interpretation is that since the
static correlations have no energy difference in the denominator of the
Green’s function, they can only be imaginary thus leading to broadening,
while the energy shifting comes from the real part. In view of this I
probably agree with the statement that static correlations mean basically
splitting while dynamic basically shifting.

What do you think?

Best regards
Georg

On 15/03/2012, at 9:23 AM, Jürgen Gräfenstein jurgen-$-chem.gu.se wrote:

Your point about quasi-deneracy merits some more thought.  So, you're
suggesting that when the broadening of the energies by the correlation is
smaller than their splitting, the >correlation is "dynamic"?  Maybe a
self-energy concept can be leveraged here.



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Seth Olsen
ARC Australian Research Fellow
6-431 Physics Annexe
School of Mathematics and Physics
The University of Queensland
Brisbane QLD 4072 Australia
seth.olsen~~uq.edu.au
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