Flavone was purchased from Sigma-Aldrich chemicals
and used without
any purification. R2PI experiments have been performed employing a
molecular beam setup described previously.
35 (link) (see also Supporting Information
SI1).
Briefly, flavone was heated up to 150 °C within a glass container
in order to obtain sufficient vapor pressure and expanded using neon
at 1.5 bar as a carrier gas through a General Valve pulsed nozzle
with a 0.5 mm orifice diameter, which was kept 5 °C higher than
the main body in order to avoid clogging. After being skimmed by a
2 mm skimmer, the molecular beam entered an ionization chamber where
ions or electrons were detected using either a reflection time-of-flight
(R.M. Jordan Co.) setup for mass-resolved ion detection or a custom-built
setup (R.M. Jordan Co.) for electron detection.
(1 + 1′)
R2PI excitation spectra were recorded using a frequency-doubled
Sirah Cobra-Stretch dye laser operating on DCM/Pyrromethene 597 pumped
by a Spectra-Physics Lab 190 Nd/YAG laser for excitation and a Neweks
PSX-501 ArF excimer laser (193 nm, 6.42 eV) for ionization. Typically,
pulse energies of 10–50 μJ and 1 mJ were used for excitation
and ionization, respectively. For recording ionization threshold spectra,
the same pulsed dye laser system has been used in combination with
another pulsed dye laser system consisting of a frequency-doubled
Sirah Precision Scan dye laser operating on DCM or Pyrromethene 597
and pumped by a Spectra Physics Lab 190 Nd/YAG laser. In these experiments,
typical pulse energies were employed of 1 mJ for the pump laser and
2–4 mJ for the probe laser.
In order to analyze the observed
electronic transitions and to
determine the ionization energy of flavone and its complexes, DFT
has been used to determine the equilibrium geometries and harmonic
force fields of flavone in the electronic ground state of the neutral
(S
0) and cation (D
0), while time-dependent DFT
(TD-DFT) was employed to optimize the geometry of the molecule in
the first three electronically excited singlet states of the neutral
and to determine the associated harmonic force fields. Such calculations
have been performed at both the B3LYP/TVZP and wB97XD/cc-pVDZ level.
36 (link)−39 (link) For comparison with the experimental results, the obtained equilibrium
geometries and force fields were used to obtain Franck–Condon
spectra at wB97XD/cc-pVDZ level for S
n ← S
0 transitions for which vibrational frequencies
were scaled using a scaling factor of 0.953.
40 (link),41 All calculations have been performed with the Gaussian16, Rev.C.01
suite of programs.
42
Fan J, & Buma W.J. (2023). Resonance-Enhanced Multiphoton Ionization Studies of the Lower Electronically Excited States of Flavone. The Journal of Physical Chemistry. a, 127(7), 1649-1655.