Titlebook: Nanostructured Soft Matter; Experiment, Theory, Andrei V. Zvelindovsky Book 2007 Springer Science+Business Media B.V. 2007 Copolymer.Heliu

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Characterization of Surfactant Water Systems by X-Ray Scattering and 2H NMRy [1] but are now becoming important as a medium for the templating of nanostruc- tured materials [2-7]. Surfactants are molecules which possess two different moieties; a hydrophobic moiety and a hydrophilic moiety [8] and typically have dimensions in the range 1 to 10 nm. At very low concentrations

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Structure and Shear-Induced Order in Blends of a Diblock Copolymer with the Corresponding Homopolymen have a profound influence on their miscibility and rheology. Shear-induced mixing or demixing of polymer blends have both been observed. Shear-induced mixing is the typical behaviour of blends of low molar mass polymers and polymer solu- tions. However, shear-induced demixing can be observed for s

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Electric Field Alignment of Diblock Copolymer Thin Filmsnd _N, where _ is the Flory-Huggins segmental interaction parameter and N is the degree of polymerization [1, 2]. The sizes of the microdomains are dictated by the total molecular weight of the copolymer and, hence, are tens of nanometers in size. This size scale cannot be easily achieved using conv

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Structure and Dynamics of Cylinder Forming Block Copolymers in Thin Filmsmers. Cylinder-forming AB diblock and ABA triblock copolymers are used as model systems. In the introduction we briefly describe the physics which commonly governs block copolymer phase behavior both in bulk and in thin films; then we define characteristic features of thin film behavior with spe- ci

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Scaling Theory of Polyelectrolyte and Polyampholyte Micelleson properties of uncharged polymers are now reasonably well understood. How- ever, many practically important polymers, both synthetic and natural, are charged in polar solvents, most commonly in water. The added complexity of charged systems stems from their long-range electrostatic interactions. T

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