Exact ground states of two-dimensional Ising spin glasses with Gaussian and
bimodal (+/-J) distributions of the disorder are calculated using a "match
ing" algorithm, which allows large system sizes of up to N=480(2) spins to
be investigated. We study domain walls induced by two rather different type
s of boundary condition changes, and, in each case, analyze the system-size
dependence of an appropriately defined "defect energy," which we denote by
AE. For Gaussian disorder, we find a power-law behavior DeltaE similar toL
(theta), with theta = -0.266(2) and theta = -0.282( 2) for the two types of
boundary condition changes. These results are in reasonable agreement with
each other. allowing for small systematic effects. They also agree well wi
th earlier work on smaller sizes. The negative value indicates that two dim
ensions is below the lower critical dimension d(c). For the +/-J model, we
obtain a different result, namely that the domain-wall energy saturates at
a nonzero value for L --> proportional to so theta = 0, indicating that the
lower critical dimension for the +/-J model is exactly d(c) = 2.