Abstract
The trapping of a resonant phonon by a pair of paramagnetic ions is studied in the limit of zero temperature with the aid of the Heitler damping formalism. The probability amplitudes of the states (spin 1 up, spin 2 down, no phonon), (spin 1 down, spin 2 up, no phonon), and (spin 1 down, spin 2 down, one phonon) are computed. Provided coherence is maintained between the two spins, the transfer of energy to the crystal lattice takes place in the time T10(1sink0r12k0r12)1. Here T10 is the spin-lattice relaxation time for an isolated ion at zero degrees, k0 is the wave vector of the resonant phonon, and r12 is the distance between the spins. The relation of this result to the general problem of spin-lattice relaxation at low temperature is discussed.