Large static first and second hyperpolarizabilities dominated by excess electron transition for radical ion pair salts M2˙+TCNQ˙− (M = Li, Na, K)†
Abstract
The interesting radical ion pair salts M2˙+TCNQ˙− (M = Li, Na, K) are a particular class of charge transfer complexes with excess electron. The ground states of these complexes are triplet. The C2v symmetry geometrical structures of the M2˙+TCNQ˙− (M = Li, Na, K) with all-real frequencies are obtained at the density functional theory (DFT) B3LYP/6-31+G(d) level. All calculations of electric properties in this paper have been carried out at the restricted open-shell second order Møller–Plesset perturbation theory (ROMP2) level. Owing to existing excess electron (from the polarized
For these radical ion pair salts M2˙+TCNQ˙−, the static first hyperpolarizabilities (β0) are large. The order of β0 values is 19 203 (M = Li) < 24 140 (M = Na) < 29 065 a.u. (M = K). Specially, the second hyperpolarizability (γ0) of the complexes with excess electron is obtained for the first time. These static second hyperpolarizabilities are also large. The order of γ0 values is 2 213 006 (M = Li) < 3 136 754 (M = Na) < 7 905 623 a.u. (M = K). Among the three structures, K2˙+TCNQ˙− has the largest γ0 value to be 7.9 × 106 a.u. (3982 × 10−36 esu), which is about 9 times larger than that of the intramolecular charge transfer complex σ-arylvinylidene trans-[Ru(4-CCHC6H4C
CC6H4NO2)Cl(dppm)2]PF6 [Hurst et al., Organometallics, 2001, 20, 4664]. The present investigation provides a new kind of candidates for the high-performance NLO materials.