The relaxation dynamics of nanoscale molecules such as Mn12Ac arises f
rom spin-lattice coupling and interaction with nuclear spins. Using a
resolvent method in terms of the energy eigenstates and the first Born
approximation with respect to phonon scattering, and averaging over t
he hyperfine field, we obtain a controlled approximation for the non-e
quilibrium magnetic relaxation behaviour and, in particular, for the c
orresponding rate. The rate is finite at T = 0, then increases linearl
y with T, and shows Arrhenius behaviour at higher temperature; for zer
o magnetic held B there are two different activation energies. The res
onances as a function of B are shown to be slightly asymmetric about B
= 0. Taking account of a quartic crystal field gives rise to a temper
ature-dependent shift of the resonant values of B. We find that, contr
ary to previous results, the rate is independent of the magnetic field
at low but finite temperatures; for T --> 0 it is linear in B. Finall
y we compare our findings with various experimental data.