The millimeter and submillimeter-wave molecular-beam spectrum of the perdeu
terated ammonia dimer (ND3)(2) has been measured between approximately 50 a
nd 400 GHz using an electric-resonance optothermal spectrometer (EROS). As
in the case of the (NH3)(2), the spectrum is complicated by the threefold i
nternal rotation of the ND3 subunits, the interchange tunneling of the two
subunits, and the inversion of the subunits through their respective center
s of masses. These tunneling motions split the rigid-molecule energy levels
into 22 components, which all have nonzero statistical weights in the case
of the deuterated dimer. Transitions have been assigned for rotation-tunne
ling states correlating to A-A (ortho-ortho) combinations of the ND3 monome
r states, where A designates the rovibronic symmetries of the ND3 subunits.
One K=1<--1, one K=1<--0, one K=0<--1, and two K=0<--0 progressions have b
een assigned. The data have been fit to 0.28 MHz using linear molecule-type
energy-level expressions to determine rotational constants, band origins,
l/K-type double constants, and centrifugal distortion constants. The two K=
0<--0 subbands, with origins near 264 GHz, are split by 64 MHz due to monom
er inversion, as observed previously in the NH3 dimer. The 264 GHz, K=0 spl
itting arises predominantly from monomer interchange tunneling and is nearl
y a factor of 2 less than the 483 GHz value for the NH3 dimer. The separati
on is also approximately 25% smaller than predicted by Olthof et al. [E. H.
T. Olthof, A. van der Avoird, and P. E. S. Wormer, J. Chem. Phys. 101, 843
0 (1994)] from dynamical calculations on a model potential energy surface a
djusted to fit the observed far-infrared rotation-tunneling spectrum of the
NH3 dimer. (C) 1999 American Institute of Physics. [S0021-9606(99)01419-1]
.