The pH-induced swelling and collapse of a polybase brush synthesized by atom transfer radical polymerization

Soft Matter 2:12 (2006) 1076-1080

Authors:

M Geoghegan, L Ruiz-Pérez, CC Dang, AJ Parnell, SJ Martin, JR Howse, RAL Jones, R Golestanian, PD Topham, CJ Crook, AJ Ryan, DS Sivia, JRP Webster, A Menelle

Abstract:

We have used neutron reflectometry to characterize the swelling behaviour of brushes of poly[2-(diethyl amino)ethyl methacrylate], a polybase, as a function of pH. The brushes, synthesized by the "grafting from" method of atom transfer radical polymerization, were observed to approximately double their thickness in low pH solutions, although the pKa is shifted to a lower pH than in dilute solution. The composition-depth profile obtained from the reflectometry experiments for the swollen brushes reveals a region depleted in polymer between the substrate and the extended part of the brush. © The Royal Society of Chemistry.

Controlling drop size and polydispersity using chemically patterned surfaces

(2006)

Authors:

H Kusumaatmaja, JM Yeomans

Modelling contact angle hysteresis on chemically patterned and superhydrophobic surfaces

(2006)

Authors:

H Kusumaatmaja, JM Yeomans

Gauge symmetry and non-abelian topological sectors in a geometrically constrained model on the honeycomb lattice

(2006)

Authors:

Paul Fendley, Joel E Moore, Cenke Xu

Density of quasiparticle states for a two-dimensional disordered system: Metallic, insulating, and critical behavior in the class D thermal quantum Hall effect

ArXiv cond-mat/0610700 (2006)

Authors:

A Mildenberger, F Evers, AD Mirlin, JT Chalker

Abstract:

We investigate numerically the quasiparticle density of states $\varrho(E)$ for a two-dimensional, disordered superconductor in which both time-reversal and spin-rotation symmetry are broken. As a generic single-particle description of this class of systems (symmetry class D), we use the Cho-Fisher version of the network model. This has three phases: a thermal insulator, a thermal metal, and a quantized thermal Hall conductor. In the thermal metal we find a logarithmic divergence in $\varrho(E)$ as $E\to 0$, as predicted from sigma model calculations. Finite size effects lead to superimposed oscillations, as expected from random matrix theory. In the thermal insulator and quantized thermal Hall conductor, we find that $\varrho(E)$ is finite at E=0. At the plateau transition between these phases, $\varrho(E)$ decreases towards zero as $|E|$ is reduced, in line with the result $\varrho(E) \sim |E|\ln(1/|E|)$ derived from calculations for Dirac fermions with random mass.