8th Liquid Matter Conference September 6-10, 2011 Wien, Austria ...

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$Edge excitations of paired fractional quantum Hall states$

P7.28Thu 811:10-14:00Effects of anomalous diffusion of mobile charges andimpedance spectroscopy for finite-length situations insoft matterLuiz Roberto Evangelista, 1 Ervin Kaminski Lenzi, 1 Giovanni Barbero, 2 and JamesRoss Macdonald 31 Universidade Estadual de Maringá, Departamento de Física, Avenida Colombo, 5790,87010340, Maringá, Brazil2 Dipartimento di Fisica del Politecnico di Torino, Torino, Italy3 University of North Carolina, Department of Physics and Astronomy, Chapel Hill,North Carolina, United States of AmericaThe redistribution of ions in confined soft matter samples can be described in the framework ofthe Poisson-Nernst-Plank (PNP) models. A normal-diffusion treatment of this and more generalsituations appeared in 1953 [1]. Recently, two finite length fractional anomalous diffusion solvingPoisson’s equation (PNPA) models have been proposed and their responses explored [2, 3]. Inthis work, we first discuss the responses and the physical appropriateness and usefulness of thesetwo empirical, but plausible, independent generalization of PNP model incorporating anomalousdiffusion of PNPA type with power-law frequency-response elements involving fractionalexponent [4]. The first model [3] involves the common separation of the expression for ordinaryPNP impedance into an interface diffusion part and a high-frequency limiting conductance andcapacitance, followed by the replacement of all normal diffusion elements in the former byanomalous ones. The second model [2], alternatively generalizes the normal time derivatives inthe continuity equation by replacing them with fractional ones and leads to no plateau, except inthe PNP limit, but instead predicts an immediate power-law increase as the frequency decreasesbelow the Debye relaxation one. Fitting of experimental frequency response data sets leads tomuch poorer fits for the second model than for the first one. Other possibilities of generalizationare discussed, including a model that combines fractional derivatives with ordinary ones andnonlocal memory effects.[1] J. R. Macdonald, Phys. Rev. 92, 4 (1953).[2] E. K. Lenzi, L. R. Evangelista, and G. Barbero, J. Phys. Chem. B 113, 11371 (2009).[3] J. R. Macdonald, J. Phys. : Condensed Matter 22, 495101 (2010).[4] J. R. Macdonald, L. R. Evangelista, E. K. Lenzi, and G. Barbero, J. Phys. Chem. C (2011), toappear.28
Thu 811:10-14:00P7.29Coarse-grained simulations of kinetic-frictionmodification in confined complex fluidsMatthew Farrow 1 and Philip Camp 11 The University of Edinburgh, School of Chemistry, West Mains Road EH9 3JJ, Edinburgh,United KingdomLangevin dynamics using coarse-grained bead-spring model beads were used to explore kineticfrictionmodification of complex fluids confined between parallel planar walls under shear. Themodels reflect the essential solvophobic and solvophilic natures of the chemical groups that makeup the friction modifiers (additives) in base oil. The degree of friction modification was surveyedas a function of wall separation, wall sliding velocity (shear rate), additive molecular weight andarchitecture, and oil-additive composition. As a rule, the kinetic-friction was found to increasefirst linearly then logarithmically with increasing sliding velocity. The results for different additivemolecules show some subtle but systematic effects that indicate an optimum molecular weight andarchitecture for kinetic-friction modification.29
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8th Liquid Matter ConferenceSeptemb
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P1.6Fri 911:10-14:00Structure and d
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P1.8Fri 911:10-14:00Surface tension
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P1.16Fri 911:10-14:00Computer simul
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P1.28Fri 911:10-14:00Proline based
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P1.36Fri 911:10-14:00A molecular dy
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P1.38Fri 911:10-14:00The lquid-liqu
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P1.40Fri 911:10-14:00Nanoporous car
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P1.42Fri 911:10-14:00Computational
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Session 2:Water, solutions and reac
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P2.2Tue 611:23-14:00Water + tert-bu
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P2.4Tue 611:23-14:00Experimental ev
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P2.6Tue 611:23-14:00Trapping proton
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P2.16Tue 611:23-14:00Dipolar solute
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P2.24Tue 611:23-14:00Study of supra
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P2.26Tue 611:23-14:00Local thermody
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P2.28Tue 611:23-14:00Ultrasonic evi
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P2.30Tue 611:23-14:00The theoretica
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P2.32Tue 611:23-14:00High frequency
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P2.34Tue 611:23-14:00Towards a mole
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P2.36Tue 611:23-14:00Crystallizatio
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P2.38Tue 611:23-14:00A study of die
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P2.40Tue 611:23-14:00Virial equatio
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P2.42Tue 611:23-14:00Compensation e
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P2.44Tue 611:23-14:00The electric p
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P2.46Tue 611:23-14:00The hydrophobi
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P2.48Tue 611:23-14:00Treating hydro
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P2.50Tue 611:23-14:00Correlations i
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P2.52Tue 611:23-14:00Hydrogen bond
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P2.54Tue 611:23-14:00Water structur
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P2.56Tue 611:23-14:00Rationalizing
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P2.58Tue 611:23-14:00Collective beh
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P2.60Tue 611:23-14:00Solute-solvent
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P2.62Tue 611:23-14:00Anomalous beha
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P2.64Tue 611:23-14:00The micro-stru
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P2.66Tue 611:23-14:00Parameterizati
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P2.68Tue 611:23-14:00Is there a ris
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P2.70Tue 611:23-14:00Excess entropy
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P2.72Tue 611:23-14:00Solid/liquid a
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P2.74Tue 611:23-14:00Percolation li
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P2.76Tue 611:23-14:00Regularities i
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P2.78Tue 611:23-14:00A molecular dy
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P2.80Tue 611:23-14:00Complex phase
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P2.82Tue 611:23-14:00Understanding
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P2.84Tue 611:23-14:00Guanidinium in
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P2.88Tue 611:23-14:00Effects of int
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Session 3:Liquid crystalsP3
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P3.2Fri 911:10-14:00Studies in Cds-
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P3.34Fri 911:10-14:00Isotropic lasi
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P3.36Fri 911:10-14:00Effect of poly
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P3.38Fri 911:10-14:00Liquid crystal
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P3.40Fri 911:10-14:00Multiscale sim
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Session 4:Polymers, polyelectrolyte
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P4.2Fri 911:10-14:00Experiments and
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P4.4Fri 911:10-14:00Online monitori
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P4.6Fri 911:10-14:00Single chain dy
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P4.8Fri 911:10-14:00Helix specific
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P4.10Fri 911:10-14:00Exploring the
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P4.16Fri 911:10-14:00Structural stu
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P4.18Fri 911:10-14:00The Influence
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P4.22Fri 911:10-14:00Competitive ad
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P4.24Fri 911:10-14:00Initial steps
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P4.34Fri 911:10-14:00Structure and
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P4.48Fri 911:10-14:00Influence of t
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P4.52Fri 911:10-14:00Lamellae forma
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P4.54Fri 911:10-14:00Thermorheologi
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P4.58Fri 911:10-14:00Dielectric rel
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P4.60Fri 911:10-14:00Anomalous stru
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P4.62Fri 911:10-14:00Effect of addi
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P4.64Fri 911:10-14:00Large-scale mo
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P4.66Fri 911:10-14:00On the physica
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P4.68Fri 911:10-14:00Tuning protein
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Wed 711:10-14:00P5.1Using symmetry
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Wed 711:10-14:00P5.3Monte Carlo sim
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Wed 711:10-14:00P5.5Long-time dynam
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Wed 711:10-14:00P5.7The role of bou
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Wed 711:10-14:00P5.9Stability of or
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Wed 711:10-14:00P5.11Diffusive moti
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Wed 711:10-14:00P5.13Crystallizatio
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Wed 711:10-14:00P5.15Collective dyn
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Wed 711:10-14:00P5.17Calculation of
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Wed 711:10-14:00P5.19Detection of e
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Wed 711:10-14:00P5.21Bulk liquid st
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Wed 711:10-14:00P5.23Charged colloi
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Wed 711:10-14:00P5.25Dielectric res
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Wed 711:10-14:00P5.27Colloids in co
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Wed 711:10-14:00P5.29Phase behavior
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Wed 711:10-14:00P5.31Mesoscopic the
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Wed 711:10-14:00P5.33The renormaliz
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Wed 711:10-14:00P5.35When depletion
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Wed 711:10-14:00P5.37Confined dryin
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Wed 711:10-14:00P5.39Predicting cry
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Wed 711:10-14:00P5.41Competition be
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Wed 711:10-14:00P5.43Interactions b
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Wed 711:10-14:00P5.45Electrostatic
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Wed 711:10-14:00P5.47Homogeneous nu
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Wed 711:10-14:00P5.49Measuring coll
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Wed 711:10-14:00P5.51Influence of i
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Wed 711:10-14:00P5.53Particle dynam
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Wed 711:10-14:00P5.55Friction contr
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Wed 711:10-14:00P5.57Monte Carlo si
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Wed 711:10-14:00P5.59Key role of hy
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Wed 711:10-14:00P5.61The Kern-Frenk
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Wed 711:10-14:00P5.63Phase diagram
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TartagliaWed 711:10-14:00P5.65How s
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Wed 711:10-14:00P5.67Field induced
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Wed 711:10-14:00P5.69A modified sof
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Wed 711:10-14:00P5.71Three dimensio
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Wed 711:10-14:00P5.73Rod-like parti
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Wed 711:10-14:00P5.75Diffusion of c
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Wed 711:10-14:00P5.77Structure form
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Wed 711:10-14:00P5.79Effective forc
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Wed 711:10-14:00P5.81Nucleation lin
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Wed 711:10-14:00P5.85Fluctuation do
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Wed 711:10-14:00P5.89Concentration
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Wed 711:10-14:00P5.91Investigation
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Wed 711:10-14:00P5.93Arrest and dyn
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Wed 711:10-14:00P5.99Thermodynamic
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Wed 711:10-14:00P5.101Consolidation
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Wed 711:10-14:00P5.103Crystallizati
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Wed 711:10-14:00P5.105Coarse-graini
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Wed 711:10-14:00P5.107Monolayers of
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Wed 711:10-14:00P5.111Coarse graini
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Wed 711:10-14:00P5.113Structure, ph
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Wed 711:10-14:00P5.115A new model f
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Wed 711:10-14:00P5.117Dynamics in d
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Wed 711:10-14:00P5.119Phase behavio
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Wed 711:10-14:00P5.121Shear melting
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Wed 711:10-14:00P5.123Driven crysta
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Wed 711:10-14:00P5.125Patchy, fluor
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Wed 711:10-14:00P5.127Electrorheolo
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Wed 711:10-14:00P5.129Clogging and
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Wed 711:10-14:00P5.131Dynamics of l
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Wed 711:10-14:00P5.135Equilibrium p
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Wed 711:10-14:00P5.137Exploring pro
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Wed 711:10-14:00P5.139Accurate simu
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Wed 711:10-14:00P5.141Two-particle
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Wed 711:10-14:00P5.143Attraction be
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Wed 711:10-14:00P5.145Exact solutio
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Wed 711:10-14:00P5.147Self-aggregat
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Wed 711:10-14:00P5.149Kinetics of m
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Wed 711:10-14:00P5.151Light scatter
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Wed 711:10-14:00P5.153Frustrated co
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Wed 711:10-14:00P5.155Colloidal cub
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Wed 711:10-14:00P5.157Nonequilibriu
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Wed 711:10-14:00P5.159Numerical stu
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Wed 711:10-14:00P5.161Aging phenome
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Wed 711:10-14:00P5.163Depletion att
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Wed 711:10-14:00P5.167Electrostatic
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Wed 711:10-14:00P5.169Dynamical sig
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Wed 711:10-14:00P5.171Tomographic c
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Wed 711:10-14:00P5.173Colloidal mic
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Wed 711:10-14:00P5.175Effect of cro
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Wed 711:10-14:00P5.177Fluidization
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Wed 711:10-14:00P5.1792-dimensional
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Wed 711:10-14:00P5.181Thermophysica
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Session 6:Films, foams, surfactants
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P6.12Fri 911:10-14:00Studies on nan
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Page 511 and 512: Thu 811:10-14:00P7.9Physics of anti
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Page 523 and 524: Thu 811:10-14:00P7.21The role of me
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Page 527 and 528: Thu 811:10-14:00P7.25Ion specificit
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Page 535 and 536: Thu 811:10-14:00P7.33Morphological
Page 537 and 538: Thu 811:10-14:00P7.35Kinetics of fl
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Page 565 and 566: Thu 811:10-14:00P7.63Calculation of
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Thu 811:10-14:00P7.79Viscous dissip
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Thu 811:10-14:00P7.81Bouncing jets
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Thu 811:10-14:00P7.83Pair correlati
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Thu 811:10-14:00P7.85Shaping liquid
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Thu 811:10-14:00P7.87On the scaling
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Thu 811:10-14:00P7.89Adsorption of
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Thu 811:10-14:00P7.91Experimental s
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Thu 811:10-14:00P7.93Hexatic phase
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Thu 811:10-14:00P7.95Spontaneous sp
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Thu 811:10-14:00P7.97Glass transiti
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Thu 811:10-14:00P7.99Complex ions i
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Thu 811:10-14:00P7.101Coaxial cross
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Thu 811:10-14:00P7.103Ordering beha
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Thu 811:10-14:00P7.105Theory and si
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Thu 811:10-14:00P7.107The Saffman-T
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Thu 811:10-14:00P7.109Grain boundar
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Thu 811:10-14:00P7.111Unusual capil
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Thu 811:10-14:00P7.113Motion and os
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Thu 811:10-14:00P7.115Dissolution b
Page 619 and 620:
Thu 811:10-14:00P7.117Suspension of
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Thu 811:10-14:00P7.119Nucleation on
Page 623 and 624:
Thu 811:10-14:00P7.121Monte Carlo s
Page 625 and 626:
Thu 811:10-14:00P7.123Forces betwee
Page 627 and 628:
Thu 811:10-14:00P7.125Size selectiv
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Thu 811:10-14:00P7.127Structure and
Page 631:
Session 8:Supercooled liquids, glas
Page 634 and 635:
P8.2Thu 811:10-14:00Hyperacoustic r
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P8.4Thu 811:10-14:00Glass transitio
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P8.6Thu 811:10-14:00Sudden network
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P8.8Thu 811:10-14:00Metastable high
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P8.10Thu 811:10-14:00Measurements o
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P8.12Thu 811:10-14:00Time resolved
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P8.14Thu 811:10-14:00Freezing of wa
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P8.16Thu 811:10-14:00Connecting str
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P8.18Thu 811:10-14:00Multi-scale mi
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P8.20Thu 811:10-14:00Structure of c
Page 654 and 655:
P8.22Thu 811:10-14:00Nonlinear stre
Page 656 and 657:
P8.24Thu 811:10-14:00Bond order in
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P8.26Thu 811:10-14:00Structure and
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P8.28Thu 811:10-14:00Connecting dif
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P8.30Thu 811:10-14:00Vitrification
Page 664 and 665:
P8.32Thu 811:10-14:00Dynamic hetero
Page 666 and 667:
P8.34Thu 811:10-14:00A leading mode
Page 668 and 669:
P8.36Thu 811:10-14:00Factors contri
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P8.38Thu 811:10-14:00Theoretical st
Page 672 and 673:
P8.40Thu 811:10-14:00Computer simul
Page 674 and 675:
P8.42Thu 811:10-14:00Clear structur
Page 676 and 677:
P8.44Thu 811:10-14:00From ”isomor
Page 678 and 679:
P8.46Thu 811:10-14:00Presence and a
Page 680 and 681:
P8.48Thu 811:10-14:00Glass transiti
Page 682 and 683:
P8.50Thu 811:10-14:00Study of the k
Page 684 and 685:
P8.52Thu 811:10-14:00Particle corre
Page 686 and 687:
P8.54Thu 811:10-14:00Activity in su
Page 688 and 689:
P8.56Thu 811:10-14:00Avalanche exci
Page 690 and 691:
P8.58Thu 811:10-14:00Effect of size
Page 692 and 693:
P8.60Thu 811:10-14:00Gauge theory o
Page 694 and 695:
P8.62Thu 811:10-14:00Phase-separati
Page 696 and 697:
P8.64Thu 811:10-14:00Quasi-equilibr
Page 698 and 699:
P8.66Thu 811:10-14:00Bond dynamics
Page 701 and 702:
Tue 611:23-14:00P9.1Viscosity of su
Page 703 and 704:
Tue 611:23-14:00P9.3Influence of hy
Page 705 and 706:
Tue 611:23-14:00P9.5Molecular dynam
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Tue 611:23-14:00P9.7A microscopic d
Page 709 and 710:
Tue 611:23-14:00P9.9Rotation and mi
Page 711 and 712:
Tue 611:23-14:00P9.11A novel optica
Page 713 and 714:
Tue 611:23-14:00P9.13Evolution of d
Page 715 and 716:
Tue 611:23-14:00P9.15Stress oversho
Page 717 and 718:
Tue 611:23-14:00P9.17Effects of a n
Page 719 and 720:
Tue 611:23-14:00P9.19Modifying defo
Page 721 and 722:
Tue 611:23-14:00P9.21Efficiently ac
Page 723 and 724:
Tue 611:23-14:00P9.23Soft matter in
Page 725 and 726:
Tue 611:23-14:00P9.25Droplet mobili
Page 727 and 728:
Tue 611:23-14:00P9.27Cell-level can
Page 729 and 730:
Tue 611:23-14:00P9.29Active microrh
Page 731 and 732:
Tue 611:23-14:00P9.31Subdiffusive i
Page 733 and 734:
Tue 611:23-14:00P9.33Dynamics and r
Page 735 and 736:
Tue 611:23-14:00P9.35Single file di
Page 737 and 738:
Tue 611:23-14:00P9.37Complex dynami
Page 739 and 740:
Tue 611:23-14:00P9.39Dynamic approa
Page 741 and 742:
Tue 611:23-14:00P9.41On mechanism o
Page 743 and 744:
Tue 611:23-14:00P9.43Peclet number
Page 745 and 746:
Tue 611:23-14:00P9.45Heat transport
Page 747 and 748:
Tue 611:23-14:00P9.47Rheology of di
Page 749 and 750:
Tue 611:23-14:00P9.49Oscillatory fl
Page 751 and 752:
Tue 611:23-14:00P9.51Scaling equati
Page 753 and 754:
Tue 611:23-14:00P9.53Transport prop
Page 755 and 756:
Tue 611:23-14:00P9.55Simulation stu
Page 757 and 758:
Tue 611:23-14:00P9.57A rheological
Page 759 and 760:
Tue 611:23-14:00P9.59Limestone fill
Page 761 and 762:
Tue 611:23-14:00P9.61Incomplete equ
Page 763 and 764:
Tue 611:23-14:00P9.63Transition mec
Page 765 and 766:
Tue 611:23-14:00P9.65Nonequilibrium
Page 767 and 768:
Tue 611:23-14:00P9.67Phase-field mo
Page 769 and 770:
Tue 611:23-14:00P9.69Enhanced shear
Page 771 and 772:
Tue 611:23-14:00P9.71Dynamics of th
Page 773 and 774:
Tue 611:23-14:00P9.73Real-time moni
Page 775:
Tue 611:23-14:00P9.75Universal diss
Page 779 and 780:
Tue 611:23-14:00P10.1Mechanical gro
Page 781 and 782:
Tue 611:23-14:00P10.3Modeling twitc
Page 783 and 784:
Tue 611:23-14:00P10.5One-step metho
Page 785 and 786:
Tue 611:23-14:00P10.7Anesthetic mol
Page 787 and 788:
Tue 611:23-14:00P10.9Electrical res
Page 789 and 790:
Tue 611:23-14:00P10.11Entropy drive
Page 791 and 792:
Tue 611:23-14:00P10.13Curvature ind
Page 793 and 794:
Tue 611:23-14:00P10.15Enhanced diff
Page 795 and 796:
Tue 611:23-14:00P10.17New approach
Page 797 and 798:
Tue 611:23-14:00P10.19Spatial struc
Page 799 and 800:
Tue 611:23-14:00P10.21Cell motility
Page 801 and 802:
Tue 611:23-14:00P10.23Effect of bou
Page 803 and 804:
Tue 611:23-14:00P10.25Self-organiza
Page 805 and 806:
Tue 611:23-14:00P10.27Magnetic bire
Page 807 and 808:
Tue 611:23-14:00P10.29Swimming beha
Page 809 and 810:
Tue 611:23-14:00P10.31Hydrodynamica
Page 811 and 812:
Tue 611:23-14:00P10.33Hydrodynamic
Page 813 and 814:
Tue 611:23-14:00P10.35Membrane late
Page 815 and 816:
Tue 611:23-14:00P10.37Protein-prote
Page 817:
Tue 611:23-14:00P10.39Mesoscale hyd
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8th Liquid Matter Conference September 6-10, 2011 Wien, Austria ...

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