Abstract

It is shown that, in the melts of linear macromolecules, the effects of dynamic heterogeneity associated with the presence of end segments are not vanishingly small in the limit $$N \to \infty $$, where $$N$$ is the number of Kuhn segments in the macromolecule. The effect has a frequency nature, i.e., the division of the segments into “end” ones, more mobile in comparison with the “median” ones, mainly depends on the observation time. With the increase in the observation time, symmetrical growth of the “end” regions of the polymer chain occurs from both ends of the macromolecule which covers the entire macromolecule at times on the order of the terminal relaxation time. The effect generates nontrivial experimentally observed consequences. For example, the free induction decay of deuterons in monodisperse polymer melts of macromolecules should have an extended region with the exponential decay law $$g(t) \propto {{t}^{{ - \beta }}}$$, where $$\beta = 1$$ for the reptation model and $$\beta = {{(\alpha - 2)}^{{ - 1}}}$$ for isotropic renormalized Rouse models: $$\alpha > 2$$ is the exponent of the molecular weight dependence of the terminal relaxation time of macromolecules. At $$\alpha \leqslant 2$$, the influence of the effects of dynamic heterogeneity on the shape of free induction decay is weaker, although it is observable at sufficient accuracy of the measurements.

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