The frequency dependence ('dispersion') of the proton spin-lattice rel
axation times, T-1 and T-1 rho, in the laboratory and rotating frames
of reference, respectively, in melts of 'entangled' polymers was inves
tigated in the range 10(2)-10(8) Hz. The results can be characterized
by a series of three apparently universal power laws corresponding to
certain limits of polymer dynamics. The fluctuations of rotational iso
merism within the Kuhn segments were independently identified in all i
nvestigated cases by the minima of the temperature dependences of T-1.
A theory linking the memory function formalism of polymer dynamics wi
th the spin-lattice relaxation dispersion has been developed. On this
basis, Schweizer's renormalized Rouse approach of polymer dynamics can
suitably be employed for the derivation of expressions reproducing tw
o of the experimentally deduced power laws very closely. One of these
frequency dependences reflects a new short-time limit of the renormali
zed Rouse approach not yet considered up to now. In addition, the time
dependence of the mean-square segment displacements was derived for t
he same limits yielding a series of new power laws. The third (low-fre
quency) spin-lattice relaxation dispersion region has no theoretical c
ounterpart in the frame of the renormalized Rouse theory.