The high-field spin-lattice relaxation of deuterated methyl groups undergoi
ng relational tunneling is investigated theoretically. It is found that for
systems showing a tunneling frequency comparable to accessible Larmor freq
uencies the relaxation to equilibrium of the Zeeman energy does not follow
a simple exponential time dependence even in powdered samples due to a fini
te coupling to the relaxation of the tunneling system. This finding contras
ts to the high-temperature behavior of reorienting methyl groups which unde
rgo simple exponential relaxation. The nonexponentiality has its origin in
the statistical coupling of the three deuteron spins due to the Pauli princ
iple.