posted on 2019-04-04, 00:00authored byPeter
R. Franke, Joseph T. Brice, Christopher P. Moradi, Henry F. Schaefer, Gary E. Douberly
Helium-solvated ethylperoxy
radicals (CH<sub>3</sub>CH<sub>2</sub>OO<sup>•</sup>) are formed
via the in situ reaction between <sup>2</sup>A′ ethyl radical
and <sup>3</sup>Σ<sub>g</sub><sup>–</sup> dioxygen. The
reactants are captured sequentially
through the droplet pick-up technique. Helium droplets are doped with
ethyl radical via pyrolysis of di-<i>tert</i>-amyl peroxide
or <i>n</i>-propylnitrite in an effusive, low-pressure source.
An infrared spectrum of ethylperoxy, in the CH stretching region,
is recorded with species-selective droplet beam depletion spectroscopy.
Spectral assignments are made via comparisons to second-order vibrational
perturbation theory with resonances (VPT2 + K) based on coupled-cluster
full quartic force fields. Cubic and quartic force constants, evaluated
using a small basis set, are transformed into the normal coordinate
system of the higher level quadratic force constants. This transformation
procedure eliminates the mismatch between normal modes, which is a
source of error whenever normal coordinate force constants from different
levels of theory are combined. The spectrum shows signatures of both
the <i>C</i><sub>1</sub> <i>gauche</i> and <i>C</i><sub><i>s</i></sub> <i>trans</i> rotamers
in an approximate 2:1 ratio; this is despite the prediction that the <i>gauche</i> rotamer lies 44 cm<sup>–1</sup> lower on the
zero-Kelvin enthalpic potential surface for torsional interconversion.
Helium droplets are 0.4 K at equilibrium; therefore, in situ ethylperoxy
production is highly nonthermal.