  The Nucleon-Nucleon interaction in the singlet ($^1 S_0$) and triplet ($^3
S_1$) channels have been studied in the framework of Relativistic Harmonic
Model using the Resonating Group Method in Born-Oppenheimer approximation. The
full Hamiltonian consists of the kinetic energy, two body confinement
potential, confined one gluon exchange potential and one pion exchange
potential. Contribution of Confined One Gluon Exchange Potential and One Pion
Exchange Potential to the adiabatic nucleon-nucleon interaction potential is
discussed.
