  We study in Ising spin glasses the finite-size effects near the spin-glass
transition in zero field and at the de Almeida-Thouless transition in a field
by Monte Carlo methods and by analytical approximations. In zero field, the
finite-size scaling function associated with the spin-glass susceptibility of
the Sherrington-Kirkpatrick mean-field spin-glass model is of the same form as
that of one-dimensional spin-glass models with power-law long-range
interactions in the regime where they can be a proxy for the Edwards-Anderson
short-range spin-glass model above the upper critical dimension. We also
calculate a simple analytical approximation for the spin-glass susceptibility
crossover function. The behavior of the spin-glass susceptibility near the de
Almeida-Thouless transition line has also been studied, but here we have only
been able to obtain analytically its behavior in the asymptotic limit above and
below the transition. We have also simulated the one-dimensional system in a
field in the non-mean-field regime to illustrate that when the Imry-Ma droplet
length scale exceeds the system size one can then be erroneously lead to
conclude that there is a de Almeida-Thouless transition even though it is
absent.
