The three-dimensional mean spherical model with a L-layer film geometr
y, under Neumann-Neumann and Neumann-Dirichlet boundary conditions is
considered. Surafce fields h(1) and h(L). are supposed to act at the s
urfaces bounding the system. In the case of Neumann boundary condition
s a new surface critical exponent Delta(1)(sb) = 3/2 is found. It is a
rgued that this exponent corresponds to a special (surface-bulk) phase
transition in the model. The Privman-Fisher scaling hypothesis for th
e free energy is verified and the corresponding scaling functions for
both the Neumann-Neumann and Neumann-Dirichlet boundary conditions are
explicitly derived. If the layer field is applied at some distance fr
om the Dirichlet boundary, a family of critical exponents emerges: the
ir values depend on the exponent defining how the distance scales with
the finite size of the system, and interpolate continuously between t
he extreme cases Delta(1)(o) = 1/2 and Delta(1)(sb) = 3/2.