We calculate the Weyl anomaly for conformal field theories that can be
described via the adS/CFT correspondence. This entails regularizing t
he gravitational part of the corresponding supergravity action in a ma
nner consistent with general covariance. Up to a constant, the anomaly
only depends on the dimension d of the manifold on which the conforma
l field theory is defined. We present concrete expressions for the ano
maly in the physically relevant cases d = 2, 4 and 6. In d = 2 we find
for the central charge c = 3l/2G(N), in agreement with considerations
based on the asymptotic symmetry algebra of adS(3). In d = 4 the anom
aly agrees precisely with that of the corresponding N = 4 superconform
al SU(N) gauge theory. The result in d = 6 provides new information fo
r the (0; 2) theory, since its Weyl anomaly has not been computed prev
iously. The anomaly in this case grows as N-3, where N is the number o
f coincident M5 branes, and it vanishes for a Ricci-flat background.