Monte Carlo simulations have been performed to investigate the equilibrium
phase behaviour of a transverse Ising model in a thin-film geometry under t
he action of competing surface fields. This model is a classical isotropic
vector spin model with a ferromagnetic Ising Hamiltonian and a transverse f
ield applied perpendicular to the Ising z-axis. For finite values of the tr
ansverse field strength, Omega, the model displays an interface localizatio
n transition with a spontaneous magnetization of the film below a critical
temperature T-c. However, in the limit Omega --> co, no spontaneous magneti
zation of the film is observed.: In the two-phase regime, below T-c, a dege
neracy exists in the magnetization profiles across the film between states
of positive and negative total magnetization. The interface localization tr
ansition temperature lies below the bulk critical temperature of the film f
or competing surface fields.