We calculate the electric field gradient (efg) antishielding factors for th
e nuclei of HD and D-2 in their J = 0 and J = 1 states using perturbation t
heory. For J = 1, the factor depends on the m(j) state. Since the antishiel
ding factor is quite large, the effective efg felt by the nuclei can be mor
e than an order of magnitude greater than the bare efg on, say, an H atom.
Combined with NMR results on deuterium nuclei, this yields a compelling arg
ument that the isolated molecular hydrogen in a-Si:H(D) resides in sites of
approximate cubic symmetry, such as the amorphous analogue of tetrahedral
sites. We also report on a variational calculation fur axial field gradient
s of arbitrary magnitude.