XUV photoelectron spectroscopy (XPS) is a powerful methodfor investigatingthe electronic structures of molecules. However, the correct interpretationof results in the condensed phase requires theoretical models thataccount for solvation. Here we present experimental aqueous-phaseXPS of two organic biomimetic molecular switches, NAIP and p-HDIOP. These switches are structurally similar, but haveopposite charges and thus present a stringent benchmark for solvationmodels which need to reproduce the observed & UDelta;eBE = 1.1 eV differencein electron binding energy compared to the 8 eV difference predictedin the gas phase. We present calculations using implicit and explicitsolvent models. The latter employs the average solvent electrostaticconfiguration and free energy gradient (ASEC-FEG) approach. Both nonequilibriumpolarizable continuum models and ASEC-FEG calculations give verticalbinding energies in good agreement with the experiment for three differentcomputational protocols. Counterions, explicitly accounted for inASEC-FEG, contribute to the stabilization of molecular states andreduction of & UDelta;eBE upon solvation.
Ikonnikov, E., Paolino, M., Garcia-Alvarez, J.C., Orozco-Gonzalez, Y., Granados, C., Röder, A., et al. (2023). Photoelectron spectroscopy of oppositely charged molecular switches in the aqueous phase: theory and experiment. THE JOURNAL OF PHYSICAL CHEMISTRY LETTERS, 14(26), 6061-6070 [10.1021/acs.jpclett.3c00828].
Photoelectron spectroscopy of oppositely charged molecular switches in the aqueous phase: theory and experiment
Paolino, M;Olivucci, M;
2023-01-01
Abstract
XUV photoelectron spectroscopy (XPS) is a powerful methodfor investigatingthe electronic structures of molecules. However, the correct interpretationof results in the condensed phase requires theoretical models thataccount for solvation. Here we present experimental aqueous-phaseXPS of two organic biomimetic molecular switches, NAIP and p-HDIOP. These switches are structurally similar, but haveopposite charges and thus present a stringent benchmark for solvationmodels which need to reproduce the observed & UDelta;eBE = 1.1 eV differencein electron binding energy compared to the 8 eV difference predictedin the gas phase. We present calculations using implicit and explicitsolvent models. The latter employs the average solvent electrostaticconfiguration and free energy gradient (ASEC-FEG) approach. Both nonequilibriumpolarizable continuum models and ASEC-FEG calculations give verticalbinding energies in good agreement with the experiment for three differentcomputational protocols. Counterions, explicitly accounted for inASEC-FEG, contribute to the stabilization of molecular states andreduction of & UDelta;eBE upon solvation.File | Dimensione | Formato | |
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https://hdl.handle.net/11365/1243075