000187549 001__ 187549 000187549 005__ 20240619092103.0 000187549 0247_ $$2doi$$a10.1021/ma402439v 000187549 0247_ $$2ISSN$$a0024-9297 000187549 0247_ $$2ISSN$$a1520-5835 000187549 0247_ $$2WOS$$aWOS:000330543500034 000187549 037__ $$aFZJ-2015-01178 000187549 082__ $$a540 000187549 1001_ $$0P:(DE-HGF)0$$aHiroi, Takashi$$b0$$eCorresponding Author 000187549 245__ $$aMultiscale Dynamics of Inhomogeneity-Free Polymer Gels 000187549 260__ $$aWashington, DC$$bSoc.$$c2014 000187549 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article$$bjournal$$mjournal$$s1422619824_18652 000187549 3367_ $$2DataCite$$aOutput Types/Journal article 000187549 3367_ $$00$$2EndNote$$aJournal Article 000187549 3367_ $$2BibTeX$$aARTICLE 000187549 3367_ $$2ORCID$$aJOURNAL_ARTICLE 000187549 3367_ $$2DRIVER$$aarticle 000187549 520__ $$aFor precise understanding of the dynamics of gels, it is necessary to distinguish the effect of inherent cross-linking from accompanying inhomogeneity. This separation is realized by the use of inhomogeneity-free gel such as Tetra-PEG gel. We investigated the dynamics of Tetra-PEG gel by quasi-elastic scattering. Mesoscopic (length scale: ∼100 nm) motion was measured by dynamic light scattering (DLS). In addition to this scale, we used neutron spin echo (NSE) to measure microscopic (length scale: ∼1 nm) motion. From these measurements, it is revealed that the gels with no connectivity/topological inhomogeneities show the transition from Zimm mode to collective diffusion mode in larger length scale, even beyond the q-range of NSE. In addition to this, the absence of spatial inhomogeneities is reflected as disappearance of nondecay component in the intermediate dynamic structure factor. 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