4 research outputs found
Assessing <i>GW</i> Approaches for Predicting Core Level Binding Energies
Here we present a systematic study
on the performance of different <i>GW</i> approaches: <i>G</i><sub>0</sub><i>W</i><sub>0</sub>, <i>G</i><sub>0</sub><i>W</i><sub>0</sub> with linearized quasiparticle
equation (lin-<i>G</i><sub>0</sub><i>W</i><sub>0</sub>), and quasiparticle self-consistent <i>GW</i> (qs<i>GW</i>), in predicting core level binding
energies (CLBEs) on a series of representative molecules comparing
to KohnāSham (KS) orbital energy-based results. KS orbital
energies obtained using the PBE functional are 20ā30 eV lower
in energy than experimental values obtained from X-ray photoemission
spectroscopy (XPS), showing that any Koopmans-like interpretation
of KS core level orbitals fails dramatically. Results from qs<i>GW</i> lead to CLBEs that are closer to experimental values
from XPS, yet too large. For the qs<i>GW</i> method, the
mean absolute error is about 2 eV, an order of magnitude better than
plain KS PBE orbital energies and quite close to predictions from
Ī<i>S</i>CF calculations with the same functional,
which are accurate within ā¼1 eV. Smaller errors of ā¼0.6
eV are found for qs<i>GW</i> CLBE shifts, again similar
to those obtained using Ī<i>S</i>CF PBE. The computationally
more affordable <i>G</i><sub>0</sub><i>W</i><sub>0</sub> approximation leads to results less accurate than qs<i>GW</i>, with an error of ā¼9 eV for CLBEs and ā¼0.9
eV for their shifts. Interestingly, starting <i>G</i><sub>0</sub><i>W</i><sub>0</sub> from PBE0 reduces this error
to ā¼4 eV with a slight improvement on the shifts as well (ā¼0.4
eV). The validity of the <i>G</i><sub>0</sub><i>W</i><sub>0</sub> results is however questionable since only linearized
quasiparticle equation results can be obtained. The present results
pave the way to estimate CLBEs in periodic systems where ĪSCF
calculations are not straightforward although further improvement
is clearly needed
Post-B3LYP Functionals Do Not Improve the Description of Magnetic Coupling in Cu(II) Dinuclear Complexes
The accuracy of post-B3LYP functionals
is analyzed using an open-shell
database of CuĀ(II) dinuclear complexes with well-defined experimental
values of the magnetic coupling constants. This database provides
a sound open-shell training set to be used to improve the fitting
schemes in defining new functionals or when reparametrizing the existing
ones. For a large set of representative hybrid exchange-correlation
functionals, it is shown that the overall description of moderate-to-strong
antiferromagnetic interactions is significantly more accurate than
the description of ferromagnetic or weakly antiferromagnetic interactions.
In the case of global hybrids, the most reliable ones have 25ā40%
Fock exchange with SOGGA and PBE0 being the most reliable and M06
the exception. For range-corrected hybrids, the long-range corrected
CAM-B3LYP and ĻB97XD provide acceptable results, and M11 is
comparable but more erratic. It is concluded that the reliability
of the calculated values is system- and range-dependent, and this
fact introduces a serious warning on the blind use of a single functional
to predict magnetic coupling constants. Hence, to extract acceptable
magnetostructural correlations, a āstandardizationā
of the method to be used is advised to choose the optimal functional
Spin Adapted versus Broken Symmetry Approaches in the Description of Magnetic Coupling in Heterodinuclear Complexes
The performance of
a series of wave function and density functional
theory based methods in predicting the magnetic coupling constant
of a family of heterodinuclear magnetic complexes has been studied.
For the former, the accuracy is similar to other simple cases involving
homodinuclear complexes, the main limitation being a sufficient inclusion
of dynamical correlation effects. Nevertheless, these series of calculations
provide an appropriate benchmark for density functional theory based
methods. Here, the usual broken symmetry approach provides a convenient
framework to predict the magnetic coupling constants but requires
deriving the appropriate mapping. At variance with simple dinuclear
complexes, spin projection based techniques cannot recover the corresponding
(approximate) spin adapted solution. Present results also show that
current implementation of spin flip techniques leads to unphysical
results
New Series of Triply Bridged Dinuclear Cu(II) Compounds: Synthesis, Crystal Structure, Magnetic Properties, and Theoretical Study
Five new triply bridged dinuclear Cu(II) compounds have been synthesized, and their magnetic properties have been measured and characterized. The magnetic coupling constants (<i>J</i>) of these compounds plus a previously structurally characterized compound of the same type have been derived by appropriate fitting of the experimentally measured molar susceptibility variation with the temperature. Two of the compounds are ferromagnetically coupled, and three are antiferromagnetically coupled with <i>J</i> values in the [+150, ā40] cm<sup>ā1</sup> range. The validity of the structural aggregate Addisonās parameter as a qualitative magneto-structural correlation is confirmed. The origin of the magnetic interactions and the magnitude of the magnetic coupling have been analyzed by means of density functional theory-based calculations using a variety of state of the art exchange-correlation potentials. It is shown that the long-range separated LC-ĻPBE provides the overall best agreement with experiment for this family as well as for a set of previously reported hetero triply bridged dinuclear Cu(II) compounds, especially for ferromagnetic systems