  Exact solutions of the Schrodinger equation are obtained for the Rosen-Morse
and Scarf potentials with the position-dependent effective mass by appliying a
general point canonical transformation. The general form of the point canonical
transformation is introduced by using a free parameter. Two different forms of
mass distributions are used. A set of the energy eigenvalues of the bound
states and corresponding wave functions for target potentials are obtained as a
function of the free parameter.
