We study the electric-field-induced transitions in antiferroelectric liquid
crystals in a model that takes into account the intralayer elastic distort
ion, the nearest-neighbor interlayer interaction, the coupling of the spont
aneous polarization with the applied field, the dielectric anisotropy, and
the surface anchoring. We find that the field-induced phase sequence has a
critical dependence on cell thickness. For moderately thin cells (thickness
> 0.1 mum) with moderately strong anchoring (surface coupling similar to 1
0(-4) J/m(2)), the system, in departing from the initial anticlinic alignme
nt, first undergoes a continuous Freederiksz transition, then a first-order
surface boundary-layer transition, and finally a first-order or continuous
transition to a complete synclinic ordering. Reducing the cell thickness t
o less than 0.1 mum will make the Freedericksz transition and even the boun
dary-layer transition vanish.