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(1-sink₀r₁₂k₀r₁₂)^-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.
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D. L. Huber (1965) studied this question.
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