Above the upper critical dimension, the breakdown of hyperscaling is
associated with dangerous irrelevant variables in the renormalization group
formalism at least for systems with periodic boundary conditions. While these
have been extensively studied, there have been only a few analyses of
finite-size scaling with free boundary conditions. The conventional expectation
there is that, in contrast to periodic geometries, finite-size scaling is
Gaussian, governed by a correlation length commensurate with the lattice
extent. Here, detailed numerical studies of the five-dimensional Ising model
indicate that this expectation is unsupported, both at the infinite-volume
critical point and at the pseudocritical point where the finite-size
susceptibility peaks. Instead the evidence indicates that finite-size scaling
at the pseudocritical point is similar to that in the periodic case. An
analytic explanation is offered which allows hyperscaling to be extended beyond
the upper critical dimension.Comment: 23 pages, 8 figure