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trans–cis Photoisomerization of the Styrylpyridine Ligand in [Re(CO)3(2,2′-bipyridine)(t-4-styrylpyridine)]+: Role of the Metal-to-Ligand Charge-Transfer Excited States
Article first published online: 27 APR 2006
DOI: 10.1002/chem.200501082
Copyright © 2006 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim
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How to Cite
Bossert, J. and Daniel, C. (2006), trans–cis Photoisomerization of the Styrylpyridine Ligand in [Re(CO)3(2,2′-bipyridine)(t-4-styrylpyridine)]+: Role of the Metal-to-Ligand Charge-Transfer Excited States. Chem. Eur. J., 12: 4835–4843. doi: 10.1002/chem.200501082
Publication History
- Issue published online: 6 JUN 2006
- Article first published online: 27 APR 2006
- Manuscript Revised: 10 OCT 2005
- Manuscript Received: 2 SEP 2005
- Abstract
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Keywords:
- charge transfer;
- density functional calculations;
- photoisomerization;
- rhenium
Abstract
The trans-cis isomerization of the styrylpyridine carbon–carbon double bond induced by visible light irradiation in fac-[Re(CO)3(bpy)(stpy)]+ (bpy = 2,2′-bipyridine; stpy = t-4-styrylpyridine) has been investigated by means of quantum-chemical methods. The structures of the various cis and trans conformers of [Re(CO)3(bpy)(stpy)]+ have been optimized at the density functional theory (DFT) level. Three rotational conformers for the most stable trans isomer lie within 2.3 kJ mol−1 each other. The energy difference between the cis and trans isomers is 27.0 kJ mol−1. The electronic spectroscopy of the most stable conformers has been investigated by time-dependent DFT (TD-DFT) and complete active space self-consistent field/CAS second order perturbation theory (CASSCF/CASPT2) calculations. The lowest absorption bands are dominated by metal-to-ligand charge-transfer (MLCT, dRe→π*bpy) transitions calculated at about 25 000 cm−1 and by a strong intraligand 1IL (πstpy→π*stpy) transition in the near UV region. On the basis of CASSCF potential energy curves (PECs) calculated as a function of the torsion angle of the C
C bond of the styrylpyridine ligand, it is shown that the role of the low-lying MLCT states is important in the photoisomerization mechanism. In contrast to the free organic ligand, in which the singlet mechanism is operational via the 1IL (S1) and electronic ground (S0) states, coordination to the rhenium steers the isomerization to the triplet PEC corresponding to the 3IL state. From the 3ILt (t = trans) the system evolves to the perpendicular intermediate 3ILp (p = perpendicular) following a 90° rotation around the styrylpyridine C
C bond. The metal center acts as a photosensitizer because of the presence of photoactive MLCT states under visible irradiation. The position of the crossing between the 3IL and electronic ground state PEC determines the quantum yield of the isomerization process.

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