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000011980 0247_ $$2DOI$$a10.1039/B922649D
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000011980 084__ $$2WoS$$aChemistry, Physical
000011980 084__ $$2WoS$$aMaterials Science, Multidisciplinary
000011980 084__ $$2WoS$$aPhysics, Multidisciplinary
000011980 084__ $$2WoS$$aPolymer Science
000011980 1001_ $$0P:(DE-Juel1)VDB4260$$aWillner, L.$$b0$$uFZJ
000011980 245__ $$aPolymer dynamics under soft confinement in a self-assembled system
000011980 260__ $$aCambridge$$bRoyal Society of Chemistry (RSC)$$c2010
000011980 300__ $$a1559 - 1570
000011980 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article
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000011980 440_0 $$016881$$aSoft Matter$$v6$$x1744-683X$$y7
000011980 500__ $$aThe authors acknowledge the SoftComp Network of Excellence (NoE) program for support. The Basque Country Government (IT-436-07) and the Spanish Ministry of Education and Science (MAT 2007-63681) Consolider/Spanish Ministry of Education and Science are also gratefully acknowledged. We are also thankful to Dr Angel Moreno for many stimulating discussions and Dr Aurel Radulescu and Dr Marie-Sousai Appavou for assistance during the SANS experiments.
000011980 520__ $$aBlock copolymers that self-assemble into nano-structured melts provide an interesting template for soft confinement. An important question that arises is how the chain dynamics is affected in such self-assembled systems. Here we consider a system composed of poly(isoprene)-b-poly(dimethyl siloxane) (PI6-PDMS30, where the numbers indicate the molecular weight in kg mole(-1)) having a large asymmetry where the minor PI component block constitutes 19% of the total molecular weight. As shown by small angle neutron scattering (SANS), the system forms hexagonally ordered cylindrical structures composed of a PI phase (with a cylinder radius of about 6.4 nm) in a continuous PDMS matrix. Here we demonstrate using neutron spin-echo spectroscopy and careful H/D contrast matching schemes how the dynamics of single polymer chains (single chain contrast) and the interfacial dynamics of the domains can be resolved independently. This is achieved in the former "single chain contrast'' case by matching out the net domain scattering leaving only the intra chain coherent structure factor visible. In the latter "bulk contrast'' case, the protonated (h) PI and deuterated (d) PDMS domains are visible and most of the contrast comes from the small interfacial layer where h-PI/d-PDMS segments are intermixed and give rise to a significant contrast by which the fluctuations can be observed. Combining the results from the two contrast conditions, we show that the dynamics can be consistently described in terms of Rouse motion modified by the surface fluctuation and laterally restricted to 2D surface diffusion. Surprisingly, the fluctuations of the interface significantly contribute to the dynamics and the interfacial tension drives the fluctuations of a sizeable portion of the polymer chains while the dynamics is similar to Rouse motion.
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000011980 693__ $$0EXP:(DE-MLZ)KWS2-20140101$$1EXP:(DE-MLZ)FRMII-20140101$$5EXP:(DE-MLZ)KWS2-20140101$$6EXP:(DE-MLZ)NL3ao-20140101$$aForschungs-Neutronenquelle Heinz Maier-Leibnitz$$eKWS-2: Small angle scattering diffractometer$$fNL3ao$$x1
000011980 7001_ $$0P:(DE-HGF)0$$aLund, R.$$b1
000011980 7001_ $$0P:(DE-Juel1)VDB2684$$aMonkenbusch, M.$$b2$$uFZJ
000011980 7001_ $$0P:(DE-Juel1)130718$$aHolderer, O.$$b3$$uFZJ
000011980 7001_ $$0P:(DE-HGF)0$$aColmenero, J.$$b4
000011980 7001_ $$0P:(DE-Juel1)130917$$aRichter, D.$$b5$$uFZJ
000011980 773__ $$0PERI:(DE-600)2191476-X$$a10.1039/b922649d$$gVol. 6, p. 1559 - 1570$$p1559 - 1570$$q6<1559 - 1570$$tSoft matter$$v6$$x1744-683X$$y2010
000011980 8567_ $$uhttp://dx.doi.org/10.1039/B922649D
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