Randomly disordered (polydomain) liquid crystalline elastomers align under
stress above the structural glass transition T-g to form a monodomain. We s
tudy the dynamics of stress relaxation during the polydomain-monodomain (P-
M) transition analysing the results using the spin-glass nematic order conc
ept. The results for different materials show a universal ultra-slow logari
thmic behaviour, especially pronounced in the region of the P-M transition.
The data are approximated very well by an equation sigma(t) similar to sig
ma(eq)(epsilon) + A/(1 + alpha ln t). We propose a theoretical model of sel
f-retardation based on the concept of cooperative mechanical resistance for
the re-orientation of each domain, attempting to follow the soft-deformati
on pathway.