  Non-Hermitian but ${\cal PT}-$symmetric quantum system of an $N-$plet of
bosons described by the three-parametric Bose-Hubbard Hamiltonian
$H(\gamma,v,c)$ is picked up, in its special exceptional-point limit $c \to 0$
and $\gamma \to v$, as an unperturbed part of the family of generalized
Bose-Hubbard-like Hamiltonians $\mathfrak{H}(\lambda)=H(v,v,0)+\lambda\,{\cal
V}$ for which the unitarity of the perturbed system is required. This leads to
the construction of two different families of Hamiltonians
$\mathfrak{H}(\lambda)$. In the first one the number $N$ of bosons is assumed
conserved while in the second family such an assumption is relaxed. In both
cases the anisotropy of the related physical Hilbert space is shown reflected
by a highly counterintuitive but operationally realizable structure of
admissible perturbations $\lambda\,{\cal V}$.
