3 research outputs found
Efficient Calculation of the Rotational <b>g</b> Tensor from Auxiliary Density Functional Theory
The computation of the rotational <b>g</b> tensor with the
recently developed auxiliary density functional theory (ADFT) gauge
including atomic orbital (GIAO) methodology is presented. For the
rotational <b>g</b> tensor, the calculation of the magnetizability
tensor represents the most demanding computational task. With the
ADFT-GIAO methodology, the CPU time for the magnetizability tensor
calculation can be dramatically reduced. Therefore, it seems most
desirable to employ the ADFT-GIAO methodology also for the computation
of the rotational <b>g</b> tensor. In this work, the quality
of rotational <b>g</b> tensors obtained with the ADFT-GIAO methodology
is compared with available experimental data as well as with other
theoretical results at the HartreeāFock and coupled-cluster
level of theory. It is found that the agreement between the ADFT-GIAO
results and the experiment is good. Furthermore, we also show that
the ADFT-GIAO <b>g</b> tensor calculation is applicable to large
systems like carbon nanotube models containing hundreds of atom and
thousands of basis functions
Nature of Valence Transition and Spin Moment in Ag<sub><i>n</i></sub>V<sup>+</sup> Clusters
Evolution in the atomic structure,
bonding characteristics, stability,
and the spin magnetic moment of neutral and cationic Ag<sub><i>n</i></sub>V clusters has been investigated using first-principles
density functional approach with gradient corrected functional. It
is shown that at small sizes, the V 4s states hybridize with Ag states
to form 1S and 1P like superatomic orbitals, whereas the 3d states
are localized on V giving the V atom an effective valence of 1 or
2. Starting from Ag<sub>8</sub>V<sup>+</sup>, the V 3d states begin
to participate in the bonding by hybridizing with the nearly free
electron gas to form 1D superatomic orbitals increasing the V atom
effective valence toward 5. For the cationic clusters, this changing
valence results in three shell closures that lead to stable species.
These occur for cationic clusters containing 5, 7, and 14 Ag atoms.
The first two stable species correspond to filled 1S and 1P shells
in two and three dimensions with a valence of 2 for V, whereas the
closure at 14 Ag atoms correspond to filled 1S, 1P, and 1D shells
with V site exhibiting a valence of 5. The transition from filled
1S and 1P shells to filled 1S, 1P, and 1D shells is confirmed by a
quenching of the spin magnetic moment. The theoretical findings are
consistent with the observed drops in intensity in the mass spectrum
of Ag<sub><i>n</i></sub>V<sup>+</sup> clusters after 5,
7, and 14 Ag atoms