In this contribution we have summarized how it is possible to compute
the tunnelling amplitude for a spherical -brane: the process, in view of
our short discussion in the introduction, can be used to model the transition
between two different vacuum phases, one being the de Sitter
spacetime with cosmological constant
and the other
being the inflating inside of the
-brane, which is characterized
by the cosmological constant
. This computation was already
performed in four dimensions in the seminal work by Coleman and de Luccia
[1] and that result was reproduced in [3]. Here
we have carried out its generalization to arbitrary dimensions (referring to
[7] for a more detailed analysis).