We report the effect of the crystal field (CF) on the broken symmetry phase
transition (BSP) in solid parahydrogen, orthodeuterium, and hydrogen deute
ride. The CF was calculated taking into account a distortion from the ideal
HCP structure. We find that, in addition to the molecular field generated
by the coupling terms in the intermolecular potential, the Hamiltonian of t
he system contains a crystal-field term, originating from single-molecular
terms in the intermolecular potential. Ignoring the CF is the main cause of
the systematic underestimation of the transition pressure, characteristic
of published theories of the BSP transition. The distortion of the lattice
that gives rise to the negative CF in response to the applied pressure is i
n accord with the general Le Chatelier-Braun principle. (C) 1999 Published
by Elsevier Science B.V. All rights reserved.