theory (DFT)28 methods at the gradient-corrected correlation
functional PBE1PBE level.29 During the optimization processes,
the convergent values of maximum force, root-mean-square
(RMS) force, maximum displacement, and RMS displacement
were set by default. To analyze the spectroscopic properties,
eighty simple excited states of the studied compounds were
calculated by time-dependent DFT (TD-DFT) methods30 at the
PBE1PBE level on the basis of the optimized geometrical struc-
tures. The polarizable continuum model method (PCM)31 using
acetonitrile as the solvent was employed. The self-consistent
field (SCF) convergence criteria of the RMS density matrix and
maximum density matrix were set at 10−8 and 10−6 a.u., respect-
ively, in all the electronic structure calculations. The iterations of
excited states continued until the changes on energies of states
were no more than 10−7 a.u. between the iterations, and then
convergence was reached in all the excited states. In these calcu-
lations, the SDD32 basis set consisting the effective core poten-
tials (ECP) was employed for the iron, phosphorus, and sulfur
atoms, and the 6-31G(p,d)33 basis set for the remaining atoms
were used. To describe precisely the molecular properties, one
additional f-type polarization function was implemented for iron
(αf = 2.462) atom,34 and the d-type polarization function was
implemented for phosphorus (αd = 0.34), and sulfur (αd = 0.421)
atoms.35 All calculations were performed with the Gaussian 03
program package.36 Visualization of the optimized structures and
frontier molecular orbitals were performed by GaussView. The
Ros & Schuit method37 (C-squared population analysis method,
SCPA) is used to partition orbital composition.
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Acknowledgements
We thank financial support from the National Natural Science
Foundation China (Grant Nos. 20973172, 21071145 and
21101153), the National Basic Research Program of China (no.
2009CB220009), and the Provincial Natural Science Foundation
of Fujian (no. 2011J01063).
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