H. Reis et al., Calculation of macroscopic linear and nonlinear optical susceptibilities for the naphthalene, anthracene and meta-nitroaniline crystals, CHEM PHYS, 261(3), 2000, pp. 359-371
The macroscopic first- to third-order susceptibilities of naphthalene, anth
racene and meta-nitroaniline (mNA) are calculated using a rigorous local fi
eld approach. Molecular (hyper)polarizabilities used as input are determine
d by density functional theory calculations with specially designed basis s
ets and for mNA also by MP2 calculations with the 6-31++G** basis set. In t
he case of mNA, the permanent electric local field due to the surrounding d
ipoles in the crystal is taken into account for the first- and second-order
susceptibility by a self-consistent approach. The molecular dipole moment
and first hyperpolarizability of mNA are drastically changed by the permane
nt local field. In all cases the calculated first-order susceptibility comp
ares very favorably with experimental data, if the molecular response is di
stributed over all heavy atoms in the molecules. Similarly, the calculated
second-order susceptibility for mNA is in good agreement with available exp
erimental data, if the same distribution scheme is used and the permanent l
ocal field is taken into account properly. This implies that accurate value
s for the molecular second-order hyperpolarizability gamma have to be avail
able.
The anisotropic Lorentz field factor approximation yields results that are
only slightly worse than the best ones of the rigorous local field theory f
or the first-order susceptibilities, but fails for the second-order suscept
ibility of mNA, due to its incapability to describe the large effect of the
permanent local field on the first-order hyperpolarizability beta. (C) 200
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