A Mori approach to the dynamics of coupled tunnelling units in defect
crystals is presented. Transverse and longitudinal correlation functio
ns of a two-level system are given as continued fractions; the memory
kernels are evaluated in a usual decoupling approximation. Due to the
random configuration of the defects on the host lattice both two-level
splitting and relaxation rates show a broad distribution; the corresp
onding distribution function is derived for the case of a dipolar inte
raction of the defects. The theory covers both weak and strong couplin
g; the average interaction energy turns out to be the essential parame
ter. Dependence on frequency, temperature and concentration of the dyn
amical susceptibility is discussed. When passing from weak to strong c
oupling, the zero-temperature susceptibility shows a crossover from a
constant value to a decrease with the third power of inverse defect co
ncentration; there is quite a strong relaxational peak in the suscepti
bility. The theory accounts for several features observed in a recent
low-frequency experiment on KCl:Li.