Gas-phase spectroscopy of a vinylheptafulvene chromophore.

Abstract

The intrinsic spectral properties of the dihydroazulene (DHA)/vinylheptafulvene (VHF) photo/thermoswitch, free of solvent interactions, were investigated both experimentally and theoretically. A quaternary ammonium group was incorporated via an ethylene bridge to allow for the transfer of charged molecules to the gas phase by electrospray ionization, leaving the chromophore part itself neutral. Absorption by the two isomers was identified from ion dissociation (i.e., action spectroscopy) using a home-built sector instrument. Several fragment ions were observed, and dissociation occurred both at the charge tag side chain and at the chromophore unit itself. We measured an absorption band of VHF with a maximum at 430 ± 20 nm (2.9 eV ± 0.1 eV) but no band was discernible for the DHA in the visible region. This shows that little interconversion between the two isomers occurs during the electrospray and the subsequent trapping in an octopole for 25 ms; the latter is needed to produce ion bunches for spectroscopy where a pulsed laser system is used. For comparison, density functional theoretical calculations predicted lowest-energy vertical excitations of 3.33 eV to 3.48 eV for the DHA and 3.02 eV to 3.08 eV for the VHF (the ranges are based on the use of different functionals), which correspond to a maximal deviation between theory and experiment of 0.1 eV in the case of the VHF. The absorption by the bare ions is significantly blue-shifted compared to that by VHF in acetonitrile solution (2.64 eV), but similar within the experimental uncertainty to that by VHF in cyclohexane (2.78 eV); the transition, therefore has a significant charge-transfer character. Finally, we find that the absorption of two photons is needed to cause fragmentation of the VHF on the microsecond time scale, which indicates that prompt fragmentation from the electronically excited state or prior to the intramolecular vibrational redistribution of the excess energy plays no role. This is of particular importance for the use of the photosystem in advanced materials or molecular electronics where high photostability is required to allow for numerous isomerization cycles.