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The end-linking technique allows an accurate control over the
equilibrium structure of polymer networks. In agreement with
previous experiments in the literature [15,37], we observe that
network structure can be nicely described through a classical mean
field model. In addition, within the low concentration regime
studied here, where there are no self-entanglements among defects,
equilibrium properties depends on the concentration of defects,
while the relaxation spectrum is strongly affected by the average molar mass of the pendant material.
Polymer networks unavoidably contain defects that dictate their
long time dynamics. Among the wide variety of structural defects in a network, high molar mass pendant chains control the terminal
relaxation dynamics. For pendant chains, similarly to entangled
star polymer melts, the reptation process is inhibited and the
relaxational dynamics becomes driven by the arm retraction potential. However, since dynamic dilution effect, that reduces the
strength of the arm retraction potential in star melts, is absent; in
polymer networks the dynamics becomes drastically slower. Thus,
the stress relaxation process occurs under the action of the strong
arm retraction potential derived by Pearson and Helfand.
In agreement with previous experiments we have observed that long time relaxation modulus can be described by the Thirion- Chasset equation and the constants in this empirical equation can
be related to a parameters free theory that only requires knowing
the number of entanglements per pendant chain, its concentration, and the Rouse time among entanglements.

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