We apply both a scalar field theory and a recently developed transfer-matrix
method to study the stationary properties of metastability in a two-state model
with weak, long-range interactions: the N×∞
quasi-one-dimensional Ising model. Using the field theory, we find the analytic
continuation f~ of the free energy across the first-order transition,
assuming that the system escapes the metastable state by nucleation of
noninteracting droplets. We find that corrections to the field-dependence are
substantial, and by solving the Euler-Lagrange equation for the model
numerically, we have verified the form of the free-energy cost of nucleation,
including the first correction. In the transfer-matrix method we associate with
subdominant eigenvectors of the transfer matrix a complex-valued
``constrained'' free-energy density fα computed directly from the
matrix. For the eigenvector with an associated magnetization most strongly
opposed to the applied magnetic field, fα exhibits finite-range scaling
behavior in agreement with f~ over a wide range of temperatures and
fields, extending nearly to the classical spinodal. Some implications of these
results for numerical studies of metastability are discussed.Comment: 25 pages, REVTeX, 9 figures available upon request, FSU-SCRI-93-153,
accepted for publication in Phys. Rev.