Electronic structure and spectrum third-order nonlinear optics of the metal phthalocyanines PcM (M = Zn, Ni, TiO) - art. no. 125109

Citation
Wd. Cheng et al., Electronic structure and spectrum third-order nonlinear optics of the metal phthalocyanines PcM (M = Zn, Ni, TiO) - art. no. 125109, PHYS REV B, 6412(12), 2001, pp. 5109
Citations number
32
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science
Journal title
PHYSICAL REVIEW B
ISSN journal
01631829 → ACNP
Volume
6412
Issue
12
Year of publication
2001
Database
ISI
SICI code
0163-1829(20010915)6412:12<5109:ESASTN>2.0.ZU;2-T
Abstract
The electronic structures and spectra have been calculated using the INDO-s ingle- and double-excitation configuration interaction method, and followin g combination with the sum-over-states method the dynamic third-order polar izabilities in the third-harmonic generation (THG), electric-field-induced second harmonic generation, and degenerate four-wave mixing (DFWM) optical processes have been computed for the metal-phthalocyanines PcM (M = Zn, Ni, TiO). The calculated electronic structures show that the highest occupied molecular orbital (HOMO) and lowest unoccupied molecular orbital (LUMO) are exclusively formed from macrocycle pi orbitals and the negative values of the HOMO energies well reproduce the observed values of threshold ionizatio n potentials, and the obtained lowest transition energies are agreement wit h the observed values of the Q bands in PcM (M = Zn, Ni, TiO). The Q band i n the absorption spectrum is the contributions from the pi-->pi* electronic transitions and the B band seems to be more sensitive to the center metal atom. The calculated dynamic third-order polarizabilities show a correlatio n between the dispersion behavior of [gamma] and the absorption spectrum of Q band region, and the first resonance enhancement in the dispersion curve appears at one third or a half of transition energy for the THG or DFWM op tical process at ground state. Additionally, an enhancement of optical nonl inearities in excited state is presented in PcM, and it has a large enhance ment at excited state if there is a small third-order polarizability at gro und state. The calculated susceptibilities of chi(-3 omega;omega,omega,omeg a) of PcM films are agreement with the available measuring values in the or der of magnitude at an input wavelength of 1907 nm. Both the theoretical an d experimental results show the decrease in the order of PcTiO>PcZn>PcNi as the distances between the centered metal atom and N-4 plane increase in th e order of PcNi<PcZn<PcTiO. The electronic origin of the next to leading or der (NLO) response is analyzed from the state component and the frontier or bital character. The pi-->pi* charge transfers among macrocycle make the do minant contributions to the third-order NLO response for PcM (M = Zn, Ni) a nd LMCT make a substantial contribution to the third-order NLO response for PcTiO. The role of axial substitute is more important than that of centere d metal atom to the third-order NLO response in PcM.