  The J-matrix method of scattering is used to obtain analytic expressions for
the phase shift of two classes of relativistic exponential-type separable
potentials whose radial component is either of the general form r^(n-1)exp(-r)
or r^(2n)exp(-r^2), where n = 0, 1, or 2. The rank of these separable
potentials is n + 1. The nonrelativistic limit is obtained and shown to be
identical to the nonrelativistic phase shift. An exact numerical evaluation for
higher order potentials (n > 2) can also be obtained in a simple way as
illustrated for the case n = 3.
