Anisotropic imbibition on surfaces patterned with polygonal posts.

Philos Trans A Math Phys Eng Sci 369:1945 (2011) 2519-2527

Authors:

ML Blow, JM Yeomans

Abstract:

We present and interpret lattice Boltzmann simulations of thick films spreading on surfaces patterned with polygonal posts. We show that the mechanism of pinning and depinning differs with the direction of advance, and demonstrate that this leads to anisotropic spreading within a certain range of material contact angles.

Fractional Chern Insulators and the W-Infinity Algebra

(2011)

Authors:

SA Parameswaran, R Roy, SL Sondhi

Weakly Coupled Pfaffian as a Type I Quantum Hall Liquid

Physical Review Letters American Physical Society (APS) 106:23 (2011) 236801

Authors:

SA Parameswaran, SA Kivelson, SL Sondhi, BZ Spivak

Quantum quench in the transverse-field Ising chain.

Phys Rev Lett 106:22 (2011) 227203

Authors:

Pasquale Calabrese, Fabian HL Essler, Maurizio Fagotti

Abstract:

We consider the time evolution of observables in the transverse-field Ising chain after a sudden quench of the magnetic field. We provide exact analytical results for the asymptotic time and distance dependence of one- and two-point correlation functions of the order parameter. We employ two complementary approaches based on asymptotic evaluations of determinants and form-factor sums. We prove that the stationary value of the two-point correlation function is not thermal, but can be described by a generalized Gibbs ensemble (GGE). The approach to the stationary state can also be understood in terms of a GGE. We present a conjecture on how these results generalize to particular quenches in other integrable models.

Site dilution in Kitaev's honeycomb model

ArXiv 1106.0732 (2011)

Authors:

AJ Willans, JT Chalker, R Moessner

Abstract:

We study the physical consequences of site dilution in Kitaev's honeycomb model, in both its gapped and gapless phases. We show that a vacancy binds a flux of the emergent $Z_2$ gauge field and induces a local moment. In the gapped phase this moment is free while in the gapless phase the susceptibility has the dependence $\chi(h)\sim\ln(1/h)$ on field strength $h$. Vacancy moments have interactions that depend on their separation, their relative sublattice, and the phase of the model. Strikingly, in the gapless phase, two nearby vacancies on the same sublattice have a parametrically larger $\chi(h)\sim(h[\ln(1/h)]^{3/2})^{-1}$. In the gapped phase, even a finite density of randomly distributed vacancies remains tractable, via a mapping to a bipartite random hopping problem. This leads to a strong disorder form of the low-energy thermodynamics, with a Dyson-type singularity in the density of states for excitations.