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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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Hansen, F. Y.
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Topics
Publications (5/5 displayed)
- 2009Structure and phase transitions of monolayers of intermediate-length n-alkanes on graphite studied by neutron diffraction and molecular dynamics simulationcitations
- 2004Slow Diffusive Motions in a Monolayer of Tetracosane Molecules Adsorbed on Graphitecitations
- 2002"Slow" Diffusive Motions in Tetracosane Monolayers Adsorbed on Graphite
- 2001Monolayer Structure of the n-Alkane Tetracosane
- 2001X-ray Specular Reflectivity Study of an n-Alkane Film, Dotriacontane, Adsorbed on Si(100) Substrates
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document
Slow Diffusive Motions in a Monolayer of Tetracosane Molecules Adsorbed on Graphite
Abstract
Monolayers of intermediate-length alkane molecules such as tetracosane (n-C<SUB>24</SUB>H<SUB>50</SUB> or C24) serve as prototypes for studying the interfacial dynamics of more complex polymers, including bilayer lipid membranes. Using high-resolution quasielastic neutron scattering (QNS) and exfoliated graphite substrates, we have investigated the relatively slow diffusive motion in C24 monolayers on an energy/time scale of ∼1-36 μeV (∼0.1-4 ns). Upon heating, we first observe QNS in the crystalline phase at ∼160 K. From the crystalline-to-smectic phase transition at ∼215 K to a temperature of ∼230 K, we observe the QNS energy width to be dispersionless, consistent with molecular dynamics simulations showing rotational motion of the molecules about their long axis. At 260 K, the QNS energy width begins to increase with wave vector transfer, suggesting onset of nonuniaxial rotational motion and bounded translational motion. We continue to observe QNS up to the monolayer melting temperature at ∼340 K where our simulations indicate that the only motion slow enough to be visible within our energy window results from the creation of gauche defects in the molecules....