Ground and excited states of zinc phthalocyanine studied by density functional methods

Citation
G. Ricciardi et al., Ground and excited states of zinc phthalocyanine studied by density functional methods, J PHYS CH A, 105(21), 2001, pp. 5242-5254
Citations number
52
Categorie Soggetti
Physical Chemistry/Chemical Physics
Journal title
JOURNAL OF PHYSICAL CHEMISTRY A
ISSN journal
10895639 → ACNP
Volume
105
Issue
21
Year of publication
2001
Pages
5242 - 5254
Database
ISI
SICI code
1089-5639(20010531)105:21<5242:GAESOZ>2.0.ZU;2-9
Abstract
The first time-dependent DFT study of the excited states of ZnPc is present ed. The theoretical results provide an accurate description of the UV-vis a nd vacuum-UV spectra and prove to be in excellent agreement with gas-phase spectra and generally in line with deconvolution analyses of solution and A r/matrix absorption and MCD spectra. The nature and intensity of the main s pectral features are highlighted and interpreted on the basis of the ground state electronic structure of the complex. A fragment approach where the f our benzopyrrole rings and the aza bridges are taken as building blocks has proven to be a very important tool to fully understand the energy and comp osition of the MOs involved in the transitions and, from these, the excitat ion energies and intensities. The Gouterman a(1u) orbital is the HOMO and t he assignment of the Q band is conventional and uncontroversial. The B band comprises five E-u excitations, whose positions and intensities are in ver y good accordance with the deconvolution of the experimental absorption ban d performed with the help of MCD spectra. However, this deconvolution invok es Jahn-Teller splitting of the E-u states which we have not calculated. We find at the red edge of the B band the weak 2nd pi --> pi* transition and at the blue edge the weak n --> pi* transition which have been identified i n the experiments. We do not confirm at low energy, in the tail of the Q ba nd (the ("Q(02)") region) an electronic origin for the band which has been suggested to arise from the lowest z-polarized n --> pi* transition. This t ransition is predicted by our calculations to be very weak and to lie in th e B band region. The energies and intensities of the higher excitations are in excellent agreement with the UV N and L bands and with the far UV C and X bands. The predicted level pattern of the lowest triplet excited states fits in with phosphorescence data available and excited-state absorption sp ectra.