A quantum realization of the relativistic Harmonic oscillator is achieved i
n terms of the spatial variable x and -i (h) over bar d/dx (the minimal can
onical representation). The Hamiltonian operator is found (at lower order)
by using a perturbative expansion in the constant c(-1). Unlike the Foldy-W
outhuysen version of the relativistic hydrogen atom, conventional perturbat
ion theory cannot be applied and a perturbation of the scalar product itsel
f is required to make the theory unitary.