Vibration-rotation-tunnelling (VRT) splittings have been computed for
the dimer (NH3)(2) by the use of four different model potentials, whic
h have different barriers to internal rotations and to the interchange
of the donor and the acceptor in the hydrogen bond. The six-dimension
al nuclear motion problem is solved variationally for J = 0 and J = 1
in a symmetry adapted basis consisting of analytic radial functions an
d rigid rotor functions depending on the five internal angles. Dipole
moments, nuclear quadrupole splittings and the amount of quenching of
the monomer umbrella inversions are also computed. Good agreement with
the experimental data available for (NH3)(2) is obtained for a potent
ial that has an equilibrium hydrogen-bonded structure close to linear,
but a low interchange barrier (24 cm(-1)). Although even the mixed or
tho-para states have large amplitude motions with this potential, our
calculations on (ND3)(2) still explain the near absence of shifts in t
he nuclear quadrupole splittings and the observed change in the dipole
moment upon isotope substitution.