Abstract— –Spectral properties of isoalloxazines in organic solvents of low polarity are determined at 300 and 77 K. Vibrational structure in the spectra reveals a vibrational mode of 1250cm‐. The pure electronic transition energies are established to a greater accuracy than was done previously and comparison to theoretical data is made. Actual lifetimes up to 10 ns for fluorescence and 300 ms for phosphorescence are found. The ratio of the actual fluorescence lifetime and the radiative lifetime is found to agree well with the quantum yield. Solvent interactions hardly shift the energy of the first electronically excited singlet state but merely affect the Franck‐Condon envelope of the spectrum and the non radiative decay of the chromophore. In albne solutions at 77 K isoalloxazine clusters are formed exhibiting P‐type delayed fluorescence.
The lowest excited singlet states of the structurally rigid amines
1-azaadamantane and 1-azabicyclo[2.2.2]octane have been investigated by using fluorescence excitation
spectroscopy on samples seeded in supersonic
expansions. Based upon the notion that in both species the lowest
excited singlet state is a Rydberg state with the
ground state of the radical cation as its ionic core, excitation
spectra have been analyzed by employing density
functional calculations of the equilibrium geometries and force fields
of the ground state of the neutral species and
its radical cation. A good agreement is obtained between
experimentally observed and theoretically predicted
frequencies and intensities of vibronic transitions. Subsequent
refinements of the geometry of the lowest excited
singlet state are shown to account adequately for the minor differences
between experiment and the computational
results obtained by using the radical cation as a model for the lowest
excited singlet state. From our analysis it also
becomes apparent that the excited state is in both molecules subject to
vibronic coupling with higher-lying excited
states, as exemplified by the presence of transitions to non-totally
symmetric vibrational levels. The results of the
present study enable the determination of mode-specific reorganization
energies accompanying ionization of
1-azaadamantane, which are shown to correspond qualitatively well with
those determined in resonance Raman
studies on the charge transfer transition in the electron
donor−acceptor system 1, which contains
1-azaadamantane
as the electron donor unit.
The lowest excited singlet states of 4-(dimethylamino)-4′-cyanostilbene (DCS), 4-(dimethylamino)-4′nitrostilbene (DANS), and 4-di(hydroxy-ethyl)amino-4′-nitrostilbene (DANS-diol) have been investigated by high-resolution fluorescence excitation and dispersed emission spectroscopy on samples seeded in supersonic expansions. Using ab initio calculations of the harmonic force fields of the electronic ground state as a starting point for the analysis of vibrational modes and frequencies, detailed vibrational assignments of the rich line structure of the S 1 r S 0 transition in these three push-pull stilbenes are reported. From the experimental and theoretical analysis, it becomes apparent that the excitation spectra are dominated by low-frequency vibrational modes of the stilbene-like backbone, albeit that a characterization in terms of trans-stilbene vibrational terminology is not very appropriate. The fluorescence excitation and emission spectra show significant Franck-Condon factors for transitions involving these vibrational modes, in line with significant geometry changes in the stilbene moiety upon electronic excitation. Comparison of the spectroscopic data of the DANS chromophore in DANS and DANS-diol demonstrates that the inclusion of the diol auxiliary function has a significant effect on its spectroscopic properties. Similarly, the comparison between solution and gas-phase data leads to the conclusion that spectroscopic data obtained in solution for DCS allow for a reasonably good extrapolation to the isolated molecule but that the structure of DANS is, even in low-polarity solvents, already modified to a larger extent than would a priori be expected.
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