Striped States in Quantum Hall Effect: Deriving a Low Energy Theory from Hartree-Fock

(2001)

Authors:

Anna Lopatnikova, Steven H Simon, Bertrand I Halperin, Xiao-Gang Wen

Lattice Boltzmann simulations of liquid crystal hydrodynamics.

Phys Rev E Stat Nonlin Soft Matter Phys 63:5 Pt 2 (2001) 056702

Authors:

C Denniston, E Orlandini, JM Yeomans

Abstract:

We describe a lattice Boltzmann algorithm to simulate liquid crystal hydrodynamics. The equations of motion are written in terms of a tensor order parameter. This allows both the isotropic and the nematic phases to be considered. Backflow effects and the hydrodynamics of topological defects are naturally included in the simulations, as are non-Newtonian flow properties such as shear thinning and shear banding.

Oscillating sign of drag in high Landau levels

(2001)

Authors:

Felix von Oppen, Steven H Simon, Ady Stern

Phase Ordering in Nematic Liquid Crystals

(2001)

Authors:

Colin Denniston, Enzo Orlandini, JM Yeomans

Dissipation in Dynamics of a Moving Contact Line

ArXiv cond-mat/0103613 (2001)

Authors:

Ramin Golestanian, Elie Raphael

Abstract:

The dynamics of the deformations of a moving contact line is studied assuming two different dissipation mechanisms. It is shown that the characteristic relaxation time for a deformation of wavelength $2\pi/|k|$ of a contact line moving with velocity $v$ is given as $\tau^{-1}(k)=c(v) |k|$. The velocity dependence of $c(v)$ is shown to drastically depend on the dissipation mechanism: we find $c(v)=c(v=0)-2 v$ for the case when the dynamics is governed by microscopic jumps of single molecules at the tip (Blake mechanism), and $c(v)\simeq c(v=0)-4 v$ when viscous hydrodynamic losses inside the moving liquid wedge dominate (de Gennes mechanism). We thus suggest that the debated dominant dissipation mechanism can be experimentally determined using relaxation measurements similar to the Ondarcuhu-Veyssie experiment [T. Ondarcuhu and M. Veyssie, Nature {\bf 352}, 418 (1991)].