DFT/MRCI calculations on the excited states of porphyrin, hydroporphyrins,tetrazaporphyrins and metalloporphyrins

Citation
Abj. Parusel et S. Grimme, DFT/MRCI calculations on the excited states of porphyrin, hydroporphyrins,tetrazaporphyrins and metalloporphyrins, J PORPHYR P, 5(3), 2001, pp. 225-232
Citations number
41
Categorie Soggetti
Chemistry
Journal title
JOURNAL OF PORPHYRINS AND PHTHALOCYANINES
ISSN journal
10884246 → ACNP
Volume
5
Issue
3
Year of publication
2001
Pages
225 - 232
Database
ISI
SICI code
1088-4246(200103)5:3<225:DCOTES>2.0.ZU;2-7
Abstract
A combination of density functional theory and multi-reference configuratio n interaction methods (DFT/MRCI) has been applied to the calculation of ele ctronic absorption spectra in a series of porphyrin-type molecules. The cal culated excitation energies and oscillator strengths for free-base porphyri n (PH2) are in excellent agreement with experiment for both lower and highe r excited states which are characterized by a significant contribution of d ouble excitations (>20%). The 4(1)B(2u), 4(1)B(3u), and 5(1)B(2u), states a re assigned to the L-band and the 7(1)B(3u) State to the M-band. The result s for the hydroporphyrins chlorin (CH2) and bacteriochlorin (BH2) are in ag reement with the experimentally observed increase in intensity for the Q-ba nds relative to PH2. For BH2 we predict a red shift of the Q(x)-band (0.2 e V) and a blue shift of the B-band (0.5-0.7 eV) in comparison to both PH2 an d CH2. For porphyrazine (PzH(2)) and the commercial pigment phthalocyanine (PcH2) the calculated oscillator strengths of the Q-and B-bands are of comp arable size explaining the intense color of PcH2. For the metalloporphyrins with magnesium (PMg) and zinc (PZn), the x- and y-polarized components of the Q- and B-bands collapse, due to the higher D-4h symmetry of the molecul es. The calculations reproduce the slight, experimentally observed increase in the oscillator strength of the Q-band and the decrease for the B-band. These effects are ascribed to the electropositive nature of the metals rela tive to hydrogen. Except for the Q-bands, which are adequately described by the 'four-orbital model,' it is essential to account for excitations outsi de the four frontier orbitals as well as double and triple excitations for accurate reproduction of experimental data. We compare our results both wit h experiment and, where available, recent first-principle SAC-CI, MRMP, and TDDFT calculations. Copyright (C) 2001 John Wiley & Sons, Ltd.