The existence of potentials for relativistic Schrodinger operators allowing
eigenvalues embedded in the essential spectrum is a long-standing open problem.
We construct Neumann-Wigner type potentials for the massive relativistic
Schrodinger operator in one and three dimensions for which an embedded
eigenvalue exists. We show that in the non-relativistic limit these potentials
converge to the classical Neumann-Wigner and Moses-Tuan potentials,
respectively. For the massless operator in one dimension we construct two
families of potentials, different by the parities of the (generalized)
eigenfunctions, for which an eigenvalue equal to zero or a zero-resonance
exists, dependent on the rate of decay of the corresponding eigenfunctions. We
obtain explicit formulae and observe unusual decay behaviours due to the
non-locality of the operator