The low-energy ZN and AZ interactions have been studied by the method of solving the coupled-channel Schrodinger equation. Using meson-exchange potentials to represent the outer regions and a phenomenological hard core to represent the inner regions of the interactions, the zero-energy scattering lengths and phase shifts as a function of energy have been computed for various choices of coupling parameters. No bound states in these systems are indicated for the most likely values of coupling parameters and core radii.