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

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$Edge excitations of paired fractional quantum Hall states$

P5.130Wed 711:10-14:00Ultrastable superparamagnetic nanoparticle design formembrane assembly and triggered releaseErik Reimhult 11 University of Natural Resources and Life Sciences (BOKU) Vienna, Muthgasse 11,A-1190, Vienna, AustriaApplication of superparamagnetic iron oxide nanoparticles (SPIONs) as biomedical imagingcontrast agents and as actuators in smart materials, e. g. for drug delivery and release, requirethem to retain high stability even in extremely dilute suspensions, high salt and at elevatedtemperatures. These requirements can only be met by steric repulsive stabilization throughirreversibly binding, low molecular weight dispersants of e. g. poly(ethylene glycol) or a similarlyirreversibly bound organic shell which stabilizes the nanoparticle into another matrix material.We have recently demonstrated that we can stabilize SPIONs which fulfil these stability criteriausing self-assembling dispersants with nitrocatechol anchors [1]. This allows us free controlover the dispersant type by simple co-adsorption of dispersants to as-synthesized core Fe 3 O 4particles. Combined with independent control over the Fe3O4 core size in the range 3-15 nma versatile toolbox for assembly of various smart materials and for biomedical applications hasbeen created. This presentation is focussed on recent results demonstrating and characterizingstable liquid interface type assembly of such SPIONs into membranes of stealth liposomes[2]. Encapsulated molecules were released multiple times by application of short bursts ofalternating magnetic fieldsthrough a localized phase change in the membrane without heating ofthe surrounding aqueous environment. The highest efficiency of release and encapsulation wasobtained for irreversibly stabilized SPIONs with diameters ¡6 nm inserted into the lipid membrane.[1] E. Amstad et al. , Nano Lett, 9:4042 (2009).[2] E. Amstad et al. , Nano Lett, asap (2011).130
Wed 711:10-14:00P5.131Dynamics of localized particles with dynamic densityfunctional theoryJohannes Reinhardt 1 and Joseph Brader 11 University of Fribourg, Department of Physics, Chemin du Musée 3 1700, Fribourg,SwitzerlandDynamic density functional theory is a valuable tool to investigate the dynamics of colloidal systems.However, in situations with few or localized particles DDFT does not perform very well.We analyse the approximations applied in DDFT and the problems that arise with localised particles.Several methods to improve the accuracy of DDFT are presented, and their predictions arecompared to simulations for simple problem cases.131
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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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P1.10Fri 911:10-14:00Primary relaxa
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P1.12Fri 911:10-14:00An efficient m
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P1.14Fri 911:10-14:00The single par
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P1.16Fri 911:10-14:00Computer simul
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P1.18Fri 911:10-14:00Porphyrin prep
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P1.20Fri 911:10-14:00A representati
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P1.22Fri 911:10-14:00Network of tet
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P1.24Fri 911:10-14:00Inter-cation c
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P1.26Fri 911:10-14:00Atomic structu
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P1.28Fri 911:10-14:00Proline based
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P1.30Fri 911:10-14:00Magnetic prope
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P1.32Fri 911:10-14:00On peculiariti
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P1.34Fri 911:10-14:00Densities of E
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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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P1.46Fri 911:10-14:00Structural and
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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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P2.8Tue 611:23-14:00The effect of r
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P2.10Tue 611:23-14:00Equation of st
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P2.12Tue 611:23-14:00Phase transiti
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P2.14Tue 611:23-14:00Multiscale stu
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P2.16Tue 611:23-14:00Dipolar solute
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P2.18Tue 611:23-14:00Statical and d
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P2.20Tue 611:23-14:00Long-lived sub
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P2.22Tue 611:23-14:00Water-like ano
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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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P3.4Fri 911:10-14:00Undulation inst
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P3.10Fri 911:10-14:00Isotropic to n
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P3.12Fri 911:10-14:00The influence
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P3.14Fri 911:10-14:00Tuning diffusi
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P3.16Fri 911:10-14:00Instability pa
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P3.18Fri 911:10-14:00Study of new p
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P3.20Fri 911:10-14:00Stereo-specifi
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P3.22Fri 911:10-14:00Colloidal part
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P3.24Fri 911:10-14:00Polymorphism o
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P3.30Fri 911:10-14:00Spatio-tempora
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P3.32Fri 911:10-14:00Continuum theo
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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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P4.12Fri 911:10-14:00Monte Carlo si
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P4.14Fri 911:10-14:00Spherical vs p
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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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P4.20Fri 911:10-14:00Viscoelasticit
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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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P4.26Fri 911:10-14:00Diffusion of t
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P4.30Fri 911:10-14:00Slow dynamics
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P4.34Fri 911:10-14:00Structure and
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P4.36Fri 911:10-14:00Hierarchically
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P4.38Fri 911:10-14:00Microphase sep
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P4.40Fri 911:10-14:00Adsorption of
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P4.42Fri 911:10-14:00Theoretical an
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P4.44Fri 911:10-14:00Possible mecha
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P4.46Fri 911:10-14:00Monte Carlo si
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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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P4.64Fri 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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Page 377 and 378: Wed 711:10-14:00P5.113Structure, ph
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Page 381 and 382: Wed 711:10-14:00P5.117Dynamics in d
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Page 413 and 414: Wed 711:10-14:00P5.149Kinetics of m
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Wed 711:10-14:00P5.181Thermophysica
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Wed 711:10-14:00P5.183Structure of
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Wed 711:10-14:00P5.185Non-hard sphe
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Wed 711:10-14:00P5.189Criticality a
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Session 6:Films, foams, surfactants
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P6.2Fri 911:10-14:00Measurement of
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P6.4Fri 911:10-14:00Soap film motio
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P6.6Fri 911:10-14:00Water adsorptio
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P6.8Fri 911:10-14:00Roughness-enhan
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P6.10Fri 911:10-14:00Permeable shel
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P6.12Fri 911:10-14:00Studies on nan
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P6.14Fri 911:10-14:00The theoretica
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P6.16Fri 911:10-14:00Phase diagram
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P6.18Fri 911:10-14:00SAFT-gamma coa
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P6.20Fri 911:10-14:00Buckling, load
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P6.22Fri 911:10-14:00Evaluation of
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P6.24Fri 911:10-14:00Differences in
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P6.26Fri 911:10-14:00Lifetime of bu
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P6.28Fri 911:10-14:00Concentration
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P6.30Fri 911:10-14:00Nascent nanoem
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P6.32Fri 911:10-14:00Surfactant-ass
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P6.34Fri 911:10-14:00Time evolution
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P6.36Fri 911:10-14:00Mixture of PEG
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P6.38Fri 911:10-14:00Charged bilaye
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P6.40Fri 911:10-14:00Microfluidic f
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P6.44Fri 911:10-14:00Numerical simu
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Thu 811:10-14:00P7.1Dissipative par
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Thu 811:10-14:00P7.3Two-dimensional
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Thu 811:10-14:00P7.5Wall-fluid inte
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Thu 811:10-14:00P7.7Interfacial ten
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Thu 811:10-14:00P7.9Physics of anti
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Thu 811:10-14:00P7.11Diffusion phen
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Thu 811:10-14:00P7.13Water cavitati
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Thu 811:10-14:00P7.15Freezing of si
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Thu 811:10-14:00P7.17Thermodynamics
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Thu 811:10-14:00P7.19Non-equilibriu
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Thu 811:10-14:00P7.21The role of me
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Thu 811:10-14:00P7.23Computational
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Thu 811:10-14:00P7.25Ion specificit
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Thu 811:10-14:00P7.27Raman scatteri
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Thu 811:10-14:00P7.29Coarse-grained
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Thu 811:10-14:00P7.31Thickness and
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Thu 811:10-14:00P7.33Morphological
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Thu 811:10-14:00P7.35Kinetics of fl
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Thu 811:10-14:00P7.37Dielectric hea
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Thu 811:10-14:00P7.39Morphology and
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Thu 811:10-14:00P7.41The crystal-fl
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Thu 811:10-14:00P7.43Adsorption of
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Thu 811:10-14:00P7.49Complications
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Thu 811:10-14:00P7.51New method for
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Thu 811:10-14:00P7.53Numerical simu
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Thu 811:10-14:00P7.55Identifying in
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Thu 811:10-14:00P6.57Free energy of
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Thu 811:10-14:00P7.59Computing pres
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Thu 811:10-14:00P7.61Nanofluidics:
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Thu 811:10-14:00P7.63Calculation of
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Thu 811:10-14:00P7.65The effect of
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Thu 811:10-14:00P7.67Adsorption beh
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Thu 811:10-14:00P7.69Thermal capill
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Thu 811:10-14:00P7.71Aqueous electr
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Thu 811:10-14:00P7.73Critical Casim
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Thu 811:10-14:00P7.75Drag reduction
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Thu 811:10-14:00P7.77Formation of n
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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 811:10-14:00P7.91Experimental 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
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Thu 811:10-14:00P7.117Suspension of
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Thu 811:10-14:00P7.119Nucleation on
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Thu 811:10-14:00P7.121Monte Carlo s
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Thu 811:10-14:00P7.123Forces betwee
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Session 8:Supercooled liquids, glas
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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
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P8.22Thu 811:10-14:00Nonlinear stre
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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
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P8.32Thu 811:10-14:00Dynamic hetero
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P8.34Thu 811:10-14:00A leading mode
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P8.36Thu 811:10-14:00Factors contri
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P8.38Thu 811:10-14:00Theoretical st
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P8.40Thu 811:10-14:00Computer simul
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P8.42Thu 811:10-14:00Clear structur
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P8.44Thu 811:10-14:00From ”isomor
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P8.46Thu 811:10-14:00Presence and a
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P8.48Thu 811:10-14:00Glass transiti
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P8.50Thu 811:10-14:00Study of the k
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P8.52Thu 811:10-14:00Particle corre
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P8.54Thu 811:10-14:00Activity in su
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P8.56Thu 811:10-14:00Avalanche exci
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P8.58Thu 811:10-14:00Effect of size
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P8.60Thu 811:10-14:00Gauge theory o
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P8.62Thu 811:10-14:00Phase-separati
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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
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Tue 611:23-14:00P9.9Rotation and mi
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Tue 611:23-14:00P9.11A novel optica
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Tue 611:23-14:00P9.13Evolution of d
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Tue 611:23-14:00P9.15Stress oversho
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Tue 611:23-14:00P9.17Effects of a n
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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
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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
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Tue 611:23-14:00P9.41On mechanism o
Page 743 and 744:
Tue 611:23-14:00P9.43Peclet number
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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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