Abstract
The ground S6 and excited L4 states of the Mn2+ ion are perturbed by the cubic crystalline field and mixed by the spin-orbit coupling. A two-phonon Raman process, second order in the orbit-lattice interaction, is found to contribute to the ground-state splitting. The theory is developed within the framework of Van Vleck's small-wave-vector averaging procedure for acoustic phonons. Both the zero-point vibrational contribution and the temperature-dependent parts are calculated and compared with experimental measurements in Mn2+-doped MgO. Good qualitative agreement between the theory and experiment is found but quantitative agreement is not obtained.