The long-wavelength absorption band of 2,6-diphenyl-4-(2,4,6-triphenylpyridinium-1-yl) phenolate (betaine-30, B30) in ethanol and 1-chlorobutane shifts to the blue by cooling in the temperature range of 294-128 K. In addition, B30 shows fluorescence in both solvents at 77 K, which is absent at room temperature. The study of the ground and excited state of B30 and its model compound 4-(pyridinium-1-yl)-phenolate PyPo by DFT/TDDFT calculations indicates that for the perpendicular conformation, the ground state possesses a charge-separated closed-shell hole pair (hp) electronic configuration, and the S(1) state corresponds to a biradicaloid electronic structure (dd) with a small dipole moment caused by an unpaired electron on each of the orthogonal fragments. Following the absorption process, there is a driving force for geometrical relaxation within the S(1) state toward an orthogonal arrangement of the phenolate and the pyridinium ring. In this final S(1) equilibrium geometry, the energy gap between the excited and the ground state is strongly reduced and causes very efficient radiationless deactivation of the S(1) state at room temperature. At 77 K, the viscous barrier hindering large-amplitude motion enables the appearance of the fluorescence from the partially or nonrelaxed excited Franck-Condon structure. By variation of the donor and acceptor strength of the two moieties, the energy gap for perpendicular systems can be tuned, allowing, in principle, the switching between the two cases hp < dd and hp > dd. This enables a new access to the efficient construction of mnemonic systems and NLO dyes.

Gradual solvation of protons by water is observed in liquids by mixing strong mineral acids with various amounts of water in acetonitrile solutions, a process which promotes rapid dissociation of the acids in these solutions. The stoichiometry of the reaction XH(+) + n(H(2)O) = X + (H(2)O)(n)H(+) was studied for strong mineral acids (negatively charged X, X = ClO(4)¯, Cl¯, Br¯, I¯, CF(3)SO(3)¯) and for strong cationic acids (uncharged X, X = R*NH(2), H(2)O). We have found by direct quantitative analysis preference of n = 2 over n = 1 for both groups of proton transfer reactions at relatively low water concentrations in acetonitrile. At high water concentrations, we have found that larger water solvates must also be involved in the solvation of the proton while the spectral features already observed for n = 2, H(+)(H(2)O)(2), remain almost unchanged at large n values up to at least 10 M of water.

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With near-infrared gating and improved light collection geometry, the entire fluorescence band can be upconverted in a broad range of 10 000 cm−1 without readjusting optical elements, thus allowing measurements with a single pump-gate scan. Monitoring of the pump-induced white light continuum provides for the time correction of the up-converted fluorescence spectra. The overall time resolution is then limited by the pump-gate cross correlation. The technique is illustrated with the femtosecond evolution of fluorescence from two molecular probes in solution.