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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Bang, Joona
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (5/5 displayed)
- 2007Creating surfactant nanoparticles for block copolymer composites through surface chemistrycitations
- 2005Controlling self-assembly of gold nanoparticles in block copolymer templates
- 2004Origin of the thermoreversible fcc-bcc transition in block copolymer solutionscitations
- 2003Mechanisms and epitaxial relationships between close-packed and BCC lattices in block copolymer solutionscitations
- 2002Thermoreversible, Epitaxial [Formula presented] Transitions in Block Copolymer Solutionscitations
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article
Mechanisms and epitaxial relationships between close-packed and BCC lattices in block copolymer solutions
Abstract
<p>The epitaxial relationships between two close-packed lattices (face-centered cubic (fcc) and hexagonally close packed (hcp)) and the body-centered cubic (bcc) lattice of spherical micelles were investigated by small-angle X-ray scattering (SAXS) in two in situ shear cells. Two symmetric poly(styrene-b-isoprene) diblock copolymers with block molecular weights of 8.0 × 10<sup>3</sup> and 7.0 × 10<sup>3</sup> g/mol, and 1.5 × 10<sup>4</sup> and 1.5 × 10<sup>4</sup> g/mol, respectively, were employed. Thermoreversible fcc → bcc order-order transitions were identified in three styrene-selective solvents, dimethyl phthalate, diethyl phthalate and dibutyl phthalate, and in two isoprene-selective solvents, tetradecane and squalane. Upon shearing an fcc solution, a mixture of highly oriented fcc and hcp crystals was produced, due to the random stacking of the {111} planes along the shear gradient. A bcc phase was grown epitaxially from each hcp/fcc mixture by heating to a temperature within the bcc window without shear. By employing two shear cells, access to scattering along both the gradient axis and the vorticity axis was achieved. This proved crucial to elucidating both the fcc → bcc and hcp → bcc transformations. These mechanisms are related to the bain distortion and the Burgers mechanism, respectively, which are well-established in simple metals. Interestingly, the close-packed planes in fcc/hcp ({111}<sub>fcc</sub> and {0002}<sub>hcp</sub> planes) and bcc ({110} planes) were preserved during these transformations, but bcc unit cells with nine distinct orientations were produced. These reflect particular orientation relationships (ORs) between the parent fcc/hcp and the newly formed bcc crystals, which correspond to the Kurdjumov-Sachs, Burgers, Nishiyama-Wassermann, and Pitsche-Schrader ORs that are prevalent in metals.</p>