  In open double-well Bose-Einstein condensate systems which balance in- and
outfluxes of atoms and which are effectively described by a non-hermitian
PT-symmetric Hamiltonian PT-symmetric states have been shown to exist.
PT-symmetric states obey parity and time reversal symmetry. We tackle the
question of how the in- and outfluxes can be realized and introduce a hermitian
system in which two PT-symmetric subsystems are embedded. This system no longer
requires an in- and outcoupling to and from the environment. We show that the
subsystems still have PT-symmetric states. In addition we examine what degree
of detail is necessary to correctly model the PT-symmetric properties and the
bifurcation structure of such a system. We examine a four-mode matrix model and
a system described by the full Gross-Pitaevskii equation in one dimension. We
see that a simple matrix model correctly describes the qualitative properties
of the system. For sufficiently isolated wells there is also quantitative
agreement with the more advanced system descriptions. We also investigate which
properties the wave functions of a system must fulfil to allow for PT-symmetric
states. In particular the requirements for the phase difference between
different parts of the system are examined.
