6533b85efe1ef96bd12bfea0
RESEARCH PRODUCT
Anomalous Structure and Scaling of Ring Polymer Brushes
Andrey MilchevAndrey MilchevDaniel ReithKurt BinderPeter Virnausubject
chemistry.chemical_classificationQuantitative Biology::BiomoleculesCondensed Matter - Materials ScienceMaterials scienceStatistical Mechanics (cond-mat.stat-mech)Monte Carlo methodGeneral Physics and AstronomyMaterials Science (cond-mat.mtrl-sci)FOS: Physical sciencesPolymerCondensed Matter - Soft Condensed MatterRing (chemistry)GyrationMolecular physicsCondensed Matter::Soft Condensed MatterMolecular dynamicsPlanarchemistryPerpendicularSoft Condensed Matter (cond-mat.soft)ScalingCondensed Matter - Statistical Mechanicsdescription
A comparative simulation study of polymer brushes formed by grafting at a planar surface either flexible linear polymers (chain length $N_L$) or (non-catenated) ring polymers (chain length $N_R=2 N_L$) is presented. Two distinct off-lattice models are studied, one by Monte Carlo methods, the other by Molecular Dynamics, using a fast implementation on graphics processing units (GPUs). It is shown that the monomer density profiles $\rho(z)$ in the $z$-direction perpendicular to the surface for rings and linear chains are practically identical, $\rho_R(2 N_L, z)=\rho_L(N_L, z)$. The same applies to the pressure, exerted on a piston at hight z, as well. While the gyration radii components of rings and chains in $z$-direction coincide, too, and increase linearly with $N_L$, the transverse components differ, even with respect to their scaling properties: $R_{gxy}^{(L)} \propto N_L^{1/2}$, $R_{gxy}^{(R)} \propto N_L^{0.4}$. These properties are interpreted in terms of the statistical properties known for ring polymers in dense melts.
year | journal | country | edition | language |
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2011-04-26 |