Issue 11, 2009

Photophysics of phenalenone: quantum-mechanical investigation of singlet–triplet intersystem crossing

Abstract

We have examined the electronic and molecular structure of 1H-phenalen-1-one (phenalenone) in the electronic ground state and in the lowest excited states, as well as intersystem crossing. The electronic structure was calculated using a combination of density functional theory and multi-reference configuration interaction. Intersystem crossing rates were determined using Fermi’s golden rule and taking direct and vibronic spin–orbit coupling into account. The required spin–orbit matrix elements were obtained applying a non-empirical spin–orbit mean-field approximation. Our calculated electronic energies are in good agreement with experimental data. We find the lowest excited singlet states to be of the nπ* (S1) and ππ* (S2) type. Energetically accessible from S1 are two triplet states of the ππ* (T1) and nπ* (T2) type, the latter being nearly degenerate to S1. This ordering of states is retained when the molecular structure in the electronically excited states is relaxed. We expect very efficient intersystem crossing between S1 and T1. Our calculated intersystem crossing rate is ≈2 × 1010 s−1, which is in excellent agreement with the experimental value of 3.45 × 1010 s−1. Our estimated phosphorescence and fluorescence rates are many orders of magnitude smaller. Our results are in agreement with the experimentally observed behavior of phenalenone, including the high efficiency of 1O2 production.

Graphical abstract: Photophysics of phenalenone: quantum-mechanical investigation of singlet–triplet intersystem crossing

Supplementary files

Article information

Article type
Paper
Submitted
09 Sep 2008
Accepted
12 Dec 2008
First published
29 Jan 2009

Phys. Chem. Chem. Phys., 2009,11, 1688-1696

Photophysics of phenalenone: quantum-mechanical investigation of singlet–triplet intersystem crossing

M. C. Daza, M. Doerr, S. Salzmann, C. M. Marian and W. Thiel, Phys. Chem. Chem. Phys., 2009, 11, 1688 DOI: 10.1039/B815724C

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