Abstract
A detailed investigation is made of the approach to equilibrium of system of spins with I=12. The spin-spin interaction ΣkΣj<kBjkσxjσxk with Bjk constant is treated exactly, while the additional interaction ΣkΣj<kLjkσxjσxk with Ljk depending on lattice vibrations is treated by means of the assumption of sufficiently short correlation times for the Ljk operators. All correlations between the Ljk are included. The effect of the correlations usually neglected is expressed in terms of a sum over states somewhat resembling an Ising-model partition function with the time replacing interaction strength. The oscillatory relaxation via the Bjk and the monotonic relaxation via the phonons compete with each other; interference effects between the two relaxation modes also occur; the origin and nature of the irreversibility are very different for the two relaxation modes.