Mesoscale modeling of contact line dynamics

COMPUT PHYS COMMUN 122 (1999) 236-239

Authors:

D Grubert, JM Yeomans

Abstract:

We outline the lattice Boltzmann approach to modeling complex fluids and discuss where it can provide additional information to more conventional macroscopic or microscopic simulations. The method is illustrated by considering contact line dynamics in a binary fluid. (C) 1999 Elsevier Science B.V. All rights reserved.

On the 3-particle scattering continuum in quasi one dimensional integer spin Heisenberg magnets

(1999)

Airy Functions in the Thermodynamic Bethe Ansatz

Letters in Mathematical Physics Springer Nature 49:3 (1999) 229-233

The fate of spinons in spontaneously dimerised spin-1/2 ladders

(1999)

Authors:

Dave Allen, Fabian HL Essler, Alexander A Nersesyan

Short-Range Interactions and Scaling Near Integer Quantum Hall Transitions

ArXiv cond-mat/9906454 (1999)

Authors:

Ziqiang Wang, Matthew PA Fisher, SM Girvin, JT Chalker

Abstract:

We study the influence of short-range electron-electron interactions on scaling behavior near the integer quantum Hall plateau transitions. Short-range interactions are known to be irrelevant at the renormalization group fixed point which represents the transition in the non-interacting system. We find, nevertheless, that transport properties change discontinuously when interactions are introduced. Most importantly, in the thermodynamic limit the conductivity at finite temperature is zero without interactions, but non-zero in the presence of arbitrarily weak interactions. In addition, scaling as a function of frequency, $\omega$, and temperature, $T$, is determined by the scaling variable $\omega/T^p$ (where $p$ is the exponent for the temperature dependence of the inelastic scattering rate) and not by $\omega/T$, as it would be at a conventional quantum phase transition described by an interacting fixed point. We express the inelastic exponent, $p$, and the thermal exponent, $z_T$, in terms of the scaling dimension, $-\alpha < 0$, of the interaction strength and the dynamical exponent $z$ (which has the value $z=2$), obtaining $p=1+2\alpha/z$ and $z_T=2/p$.