  The Dirac Equation is solved approximately for relativistic generalized
Woods-Saxon potential including Coulomb-like tensor potential in exact
pseudospin and spin symmetry limits. The bound states energy eigenvalues are
found by using wavefunction boundary conditions, and corresponding radial
wavefunctions are obtained in terms of hypergeometric function. Some numerical
examples are given for the dependence of bound states energy eigenvalues on
quantum numbers and potential parameters.
