We present an explicit study of the holographic renormalization group (RG)
in six dimensions using minimal gauged supergravity. By perturbing the theo
ry with the addition of a relevant operator of dimension four one flows to
a non-supersymmetric conformal fixed point. There are also solutions descri
bing non-conformal vacua of the same theory obtained by giving an expectati
on value to the operator. One such vacuum is supersymmetric and is obtained
by using the true superpotential of the theory. We discuss the physical ac
ceptability of these vacua by applying the criteria recently given by Gubse
r for the four-dimensional case and find that those criteria give a clear p
hysical picture in the six-dimensional case as well. We use this example to
comment on the role of the Hamilton-Jacobi equations in implementing the R
G. We conclude with some remarks on AdS(4) and the status of three-dimensio
nal superconformal theories from squashed solutions of M-theory.