The relaxation of the magnetization in big molecular groups embedded in crystals is studied and compared with experimental data on Mn 12 O 12. At sufficiently high temperatures (T > 2 K in Mn 12 O 12) the relaxation is thermally activated, and the exchange of energy with phonons produces relaxation through a cascade of elementary transitions where the component Sz of the spin along the tetragonal axis changes by δm = ±1 or ±2. At lower temperatures, tunneling occurs, but energy conservation requires exchange of energy with nuclear spins in very low magnetic fields (smaller than the hyperfine field), or with phonons in higher field. The phonon assisted tunneling rate 1/τ is proportional to H 3 for weak fields H(H < 2 Tesla ). A minimum of τ is expected when the field is of the order of magnitude of the maximum hyperfine field. The theoretically predicted minimum is sharper and should occur at a field value four times as small than experimentally observed.
In a magnetic medium the nuclear spins are coupled by the Suhl-Nakamura indirect interaction. This interaction is weak but has a very long range b. It is known to contribute to the nuclear spin relaxation. It also gives rise to a displacement of the nuclear magnetic resonance frequency which is important at temperatures in the helium range for materials with a large concentration of nuclei and large b. More generally the indirect interaction gives rise to a spectrum of nuclear spin waves. This spectrum may be shown to be meaningful even when the nuclei are far from order because of the long range of the interaction. Different methods to observe this spectrum are discussed.3 P. G. DeGennes, F. Hartmann-Boutron, and P. A. Pincus, Compt. Rend. 254, 1264 (1962. 1105
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