In this work we present calculated absorption and emission spectra in acetonitrile (MeCN) solution of N-acetyl-1-aminopyrene (PAAc, a spectroscopic model compound) and N-(1-pyrenyl)-1-methyluracil-5-carboxamide (PAU Me , a computational model for 5-(N-carboxyl-1-aminopyrenyl)-2′-deoxyuridine (PAdU)). The computational method usedsthe discrete reaction field approach (DRF)scombines a quantum mechanical (QM) description of the solute (here DFT and INDOs/CIS, i.e., the INDO parametrization for spectroscopy) with a classical, molecular mechanics (MM) description of the solvent molecules. The latter are modeled with point charges representing the permanent charge distribution and polarizabilities to account for many-body interactions among the solute and other solvent molecules. Molecular dynamics is used to sample the degrees of freedom of the solution around several solute conformations each in two electronic excited states. This leads to a large number of solute/solvent configurations from which 800 are selected for each excited state and collected into a single ensemble by means of proper Boltzmann averaging. DRF INDOs/CIS applied to the selected solute/solvent configurations give simulated absorption and emission band spectraseach based on 15 200 calculated transitionssthat compare well with experimental results. For example, the much broader absorption and emission bands in PAdU compared with PAAc are reproduced, and the simulated emission spectra of PAU Me agree well with broad (380-550 nm) charge transfer (CT) emission seen for PAdU in MeCN. The observed multiexponential fluorescence decay profiles for PAdU in different polar solvents are interpreted in terms of solute/solvent conformational heterogeneity here generated in the MD simulations for PAU Me in MeCN. Additionally, the simulations demonstrate the mixing of the forbidden Py •+ /dU •-CT states with allowed pyrenyl 1 (π,π*) states.
IntroductionThe spectroscopy of 5-(N-carboxyl-1-aminopyrenyl)-2′-deoxyuridine (PAdU; see Figure 1) in tetrahydrofuran (THF), methanol (MeOH) and acetonitrile (MeCN) 1 has several remarkable features, the most important being the extensive quenching of the photoexcited 1 (π,π*) state of its pyrenyl chromophore relative to N-acetyl-1-aminopyrene (PAAcsa spectroscopic model compound). Stronger pyrenyl emission quenching in the more polar solvents MeCN and MeOH compared to that seen in the less polar solvent THF is consistent with the proposal that the photophysics is controlled by the formation of intramolecular Py •+ /dU •-charge transfer (CT) excited states.Earlier efforts to elucidate the solvent dependence of intramolecular CT quenching of pyrenyl emission in pyrenyl-dU nucleosides by means of INDOs/CIS, i.e., the INDO parametrization for spectroscopy and wave function expansions in terms of determinants obtained from single excitation transitions only, 3 quantum chemical calculations on PAAc and a computational model for PAdU (PAU Me ; see Figure 1), were only partly satisfying in the sense that gas phase calculations 1 in...