Ju. Grabow et al., MICROWAVE-SPECTRUM, LARGE-AMPLITUDE MOTIONS, AND AB-INITIO CALCULATIONS FOR N2O5, The Journal of chemical physics, 105(17), 1996, pp. 7249-7262
The rotational spectrum of dinitrogen pentoxide (N2O5) has been invest
igated between 8 to 25 GHz at a rotational temperature of similar to 2
.5 K using a pulsed-molecular-beam Fourier-transform microwave spectro
meter. Two weak b-dipole spectra are observed for two internal-rotor s
tates of the molecule, with each spectrum poorly characterized by an a
symmetric-rotor Hamiltonian, The observation of only b-type transition
s is consistent with the earlier electron-diffraction results of McCle
lland et al. [J. Am, Chem. Sec. 105, 3789 (1983)] which give a C-2 sym
metry molecule with the b inertial axis coincident with the C-2 axis.
Analysis of the N-14 nuclear hyperfine structure demonstrates that the
two nitrogen nuclei occupy either structurally equivalent positions o
r are interchanging inequivalent structural positions via tunneling or
internal rotation at a rate larger than similar to 1 MHz. For the two
internal rotor states, rotational levels with K-a + K-c even have I-N
= 0, 2, while levels with K-a + K-c odd have I-N = 1, where I-N is th
e resultant nitrogen nuclear spin, This observation establishes that t
he equilibrium configuration of the molecule has a twofold axis of sym
metry. Guided by ab initio and dynamical calculations which show a pla
nar configuration is energetically unfavorable, we assign the spectrum
to the symmetric and antisymmetric tunneling states of a C-2 symmetry
N2O5 with internal rotation tunneling of the two NO2 groups via a gea
red rotation about their respective C-2 axes. Because of the Bose-Eins
tein statistics of the spin-zero oxygen nuclei, which require that the
rotational-vibrational-tunneling wave functions be symmetric for inte
rchange of the O nuclei, only four of the ten vibrational-rotational-t
unneling states of the molecule have nonzero statistical weights. Mode
l dynamical calculations suggest that the internal-rotation potential
is significantly more isotropic than implied by the electron-diffracti
on analysis. (C) 1996 American Institute of Physics.