Abstract
Raman scattering studies of the J=02 rotational transitions in solid parahydrogen and orthodeuterium over the pressure range 0<~p<~3.3 kbar have revealed a phase transition from hcp to fcc, with the fcc structure being stable at high pressures and hcp stable at low pressures (≲ 0.8 kbar). In both phases the main anisotropic interaction is molecular electric quadrupole-quadrupole (R5), but we observe significant effects tentatively attributed to correlated zero-point motion.