  Within the framework of quantum mechanics working with one-dimensional,
manifestly non-Hermitian Hamiltonians $H=T+V$ the traditional class of the
exactly solvable models with local point interactions $V=V(x)$ is generalized.
The consequences of the use of the nonlocal point interactions such that $(V
f)(x) = \int K(x,s) f(s) ds$ are discussed using the suitably adapted formalism
of boundary triplets.
