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024 7 _ |2 DOI
|a 10.1039/B922649D
024 7 _ |2 WOS
|a WOS:000275947800026
024 7 _ |2 MLZ
|a WillnerLMHCR2010
037 _ _ |a PreJuSER-11980
041 _ _ |a eng
082 _ _ |a 530
084 _ _ |2 WoS
|a Chemistry, Physical
084 _ _ |2 WoS
|a Materials Science, Multidisciplinary
084 _ _ |2 WoS
|a Physics, Multidisciplinary
084 _ _ |2 WoS
|a Polymer Science
100 1 _ |0 P:(DE-Juel1)VDB4260
|a Willner, L.
|b 0
|u FZJ
245 _ _ |a Polymer dynamics under soft confinement in a self-assembled system
260 _ _ |a Cambridge
|b Royal Society of Chemistry (RSC)
|c 2010
300 _ _ |a 1559 - 1570
336 7 _ |a Journal Article
|0 PUB:(DE-HGF)16
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336 7 _ |a ARTICLE
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336 7 _ |a JOURNAL_ARTICLE
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336 7 _ |a article
|2 DRIVER
440 _ 0 |0 16881
|a Soft Matter
|v 6
|x 1744-683X
|y 7
500 _ _ |a The 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.
520 _ _ |a Block 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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700 1 _ |0 P:(DE-HGF)0
|a Lund, R.
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700 1 _ |0 P:(DE-Juel1)VDB2684
|a Monkenbusch, M.
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700 1 _ |0 P:(DE-Juel1)130718
|a Holderer, O.
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700 1 _ |0 P:(DE-HGF)0
|a Colmenero, J.
|b 4
700 1 _ |0 P:(DE-Juel1)130917
|a Richter, D.
|b 5
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773 _ _ |0 PERI:(DE-600)2191476-X
|a 10.1039/b922649d
|g Vol. 6, p. 1559 - 1570
|p 1559 - 1570
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|t Soft matter
|v 6
|x 1744-683X
|y 2010
856 7 _ |u http://dx.doi.org/10.1039/B922649D
909 C O |o oai:juser.fz-juelich.de:11980
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914 1 _ |y 2010
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