Symmetry Breaking
C. David
Sherrill
School of Chemistry and
Biochemistry
Georgia Institute of
Technology
Atlanta, GA 30032-0400
Introduction
In three publications, we have presented some interesting new
results for ``symmetry breaking'' molecules. In the context of
molecular electronic structure theory, the term symmetry breaking
usually implies that a molecule turns out to have a lower point-group
symmetry than expected. In particular, degenerate electronic states
may become more stabilized by a geometrical distortion that breaks
the electronic degeneracy (the Jahn-Teller effect). Unfortunately,
however, theoretical electronic structure methods seem prone to
predicting such symmetry lowerings even when they do not occur in
reality. We term this artifactual symmetry breaking.
Thus an obvious question is how to determine whether theoretically
predicted symmetry breaking is real or artifactual. The first thing
one should examine is the symmetry of the wavefunction at
the high-symmetry geometry: if the wavefunction fails to exhibit
the full symmetry of the point group, this is a sign that predictions
of geometrical symmetry breaking may be artifactual. In such cases,
one might say that the wavefunction itself exhibits artifactual symmetry
breaking. Paradoxically, for a given approximation scheme, such
symmetry broken wavefunctions can be lower in energy (and hence
better in a variational sense) than symmetric wavefunctions, even though
the exact wavefunction must be symmetric.
This symmetry breaking problem is actually rather widespread and can
easily make a project become completely intractable. Radicals
are particularly prone to symmetry breaking and related problems.
Symmetry breaking is frequently the cause of completely unphysical
vibrational frequency predictions (e.g., frequencies of 10,000
cm-1 or more). Many users of quantum chemistry programs
probably assume that all such results are due to bugs in the code
(or failing to follow the correct solution for one of the geometries,
which frequently happens), but this is not always true: they may result
from fundamental failures in the underlying quantum mechanical models.
Symmetry Breaking and the OO-CCD Method
We found that the atmospherically important
O4+ molecule exhibits unrealistically large
vibrational frequencies at the coupled-cluster singles and doubles (CCSD)
level of theory. This is a very interesting result, since Crawford
et al. have indicated that CCSD is highly resistant to these
problems, even more so than the more complete CCSD(T) method [J. Chem.
Phys. 107, 10626 (1997)]. Using our new implementation of the
optimized-orbital coupled-cluster doubles (OO-CCD) method [J. Chem.
Phys. 109 4171 (1998);
(Abstract)], we obtain
very reasonable results. This is in accord with previous work by
Stanton et al. and by Barnes and Lindh which indicates that
Brueckner CCD (to which our OO-CCD is numerically very similar) sometimes
cleans up certain types of symmetry breaking problems.
6-31G* Geometries and Frequencies for Quartet O4+
Method | r(O-O) | r(CM)
| ag | ag | b1g
| au | b2u | b3u
|
UHF | 1.1176 | 2.4058 |
2242 | 255 | 396 | 197 | -543 |
3223 |
ROHF | 1.1152 | 2.4073 |
2256 | 258 | 417 | 199 | 83 |
3612 |
UHF CCSD | 1.1737 | 2.3792 |
1808 | 269 | 341 | 178 | 154 |
1726 |
ROHF CCSD | 1.1730 | 2.3793 |
1813 | 269 | 372 | 179 | -66 |
2036 |
B-CCD | 1.1723 | 2.3794 |
1821 | 269 | 342 | 179 | 82 |
1194 |
OO-CCD | 1.1728 | 2.3793 |
1816 | 269 | 372 | 179 | 84 |
1193 |
Expt. | | |
| | | | |
1320 |
Symmetry Breaking and
Density Functional Theory
In another paper [Chem. Phys. Lett. 302, 425 (1999);
(Abstract)], we
examined many different versions of Kohn-Sham density functional theory
(DFT) as applied to three molecules which exhibit artifactual symmetry
breaking in the unrestricted Hatree-Fock (UHF) wavefunction:
O2+, O4+, and NO3.
We found that all DFT methods considered yield symmetric
densities for each of the three molecules unless we use hybrid DFT
functionals mixing in an unusually large fraction of pure Hartree-Fock
exchange. Further tests indicated that exchange is more important than
correlation in determining whether symmetry is preserved or broken.
The above results were very encouraging and suggested that perhaps DFT may be a reliable method to use for symmetry breaking molecules. However, to test this
hypothesis, it is necessary to assess the reliability of DFT for
molecular properties (such as geometries and vibrational frequencies)
of molecules prone to artifactual symmetry breaking. We recently
published the results of such a study [J. Chem. Phys. 114, 8257 (2001);
(Abstract)].
We found that DFT appears to be among the more robust methods available
for such challenging cases, but it is still not immune to anomalous predictions for molecular properties.
This material is based in part upon work supported by the National Science
Foundation under Grant No. 0094088. Any opinions, findings, and conclusions
or recommendations expressed in this material are those of the authors and
do not necessarily reflect the views of the National Science Foundation.
© Copyright 2000 The Sherrill Group