  We investigate the Bose-Einstein Condensation on non homogeneous non amenable
networks for the model describing arrays of Josephson junctions on perturbed
Cayley Trees. The resulting topological model has also a mathematical interest
in itself. The present paper is then the application to the Bose-Einstein
Condensation phenomena, of the harmonic analysis aspects arising from additive
and density zero perturbations, previously investigated by the author in a
separate work. Concerning the appearance of the Bose-Einstein Condensation, the
results are surprisingly in accordance with the previous ones, despite the lack
of amenability. We indeed first show the following fact. Even when the critical
density is finite (which is implied in all the models under consideration,
thanks to the appearance of the hidden spectrum), if the adjacency operator of
the graph is recurrent, it is impossible to exhibit temperature locally normal
states (i.e. states for which the local particle density is finite) describing
the condensation at all. The same occurs in the transient cases for which it is
impossible to exhibit locally normal states describing the Bose--Einstein
Condensation at mean particle density strictly greater than the critical
density . In addition, for the transient cases, in order to construct locally
normal temperature states through infinite volume limits of finite volume Gibbs
states, a careful choice of the the sequence of the finite volume chemical
potential should be done. For all such states, the condensate is essentially
allocated on the base--point supporting the perturbation. This leads that the
particle density always coincide with the critical one. It is shown that all
such temperature states are Kubo-Martin-Schwinger states for a natural
dynamics. The construction of such a dynamics, which is a very delicate issue,
is also done.
