posted on 2013-10-03, 00:00authored byBérenger Gans, Guido Grassi, Frédéric Merkt
The X+ 2Π ← X 1Σ+ photoionizing transition of iodoacetylene (HC2I) has been investigated by pulsed-field-ionization zero-kinetic-energy
(PFI-ZEKE) photoelectron spectroscopy. The resolution of the rotational
structure of the spectra and its analysis provided information on
the structure of the HC2I+ cation and the photoionization
dynamics of HC2I. In the ground electronic 2Π state, the HC2I+ cation is found to
be linear and subject to a strong spin–orbit coupling. The
first adiabatic ionization energy of HC2I and the spin–orbit
splitting of the X+ 2Π ground state of HC2I+ were determined to be EI(HC2I)/hc = 78296.5(2) cm–1 and Δν̃SO = 3257(1)
cm–1, respectively. The large spin–orbit
interaction almost entirely masks the Renner–Teller effect,
which is only detectable through the observation of the nominally
forbidden transition to the first excited level (51) of
the HCC-I bending mode ν5. The interaction of ∼2
cm–1 observed between the 51 levels of 2Σ1/2 and 2Δ5/2 symmetry is attributed to a vibronic interaction with the B 2Σ+ electronic state of HC2I+. The spin–orbit energy level structure of tri- and
tetra-atomic molecules subject to the Renner–Teller effect
and spin–orbit coupling is discussed for the two limiting cases
where the spin–orbit-coupling constant is much smaller and
much larger than the bending-mode frequencies.