Joule heating of dilute 2D holes in a GaAs quantum well

(2002)

Authors:

Xuan PA Gao, Allen P Mills,, Arthur P Ramirez, Steven H Simon, Loren N Pfeiffer, Kenneth W West

Polymer induced depletion potentials in polymer-colloid mixtures

(2002)

Authors:

AA Louis, PG Bolhuis, EJ Meijer, JP Hansen

Lattice Boltzmann simulations of contact line motion in a liquid-gas system

(2002)

Authors:

AJ Briant, P Papatzacos, JM Yeomans

Spectral function of a quarter-filled one-dimensional charge density wave insulator.

Phys Rev Lett 88:9 (2002) 096403

Authors:

Fabian HL Essler, Alexei M Tsvelik

Abstract:

We consider a one-dimensional charge density wave insulator formed by umklapp processes in a quarter-filled band. The spectrum of the model consists of gapless, uncharged excitations carrying spin +/- 1/2 (spinons) and gapped, spinless excitations carrying charge -/+ signe/2 (solitons and antisolitons). We calculate the low-energy behavior of the single-electron Green's function at zero temperature. The spectral function exhibits a featureless scattering continuum of two solitons and many spinons. The theory predicts that the gap observed by angle resolved photoemission is twice the activation gap in the dc conductivity. We comment on possible applications to PrBa(2)Cu(3)O(7) and to the Bechgaard salts.

Glassy behaviour in simple kinetically constrained models: topological networks, lattice analogues and annihilation-diffusion

J PHYS-CONDENS MAT 14:7 (2002) 1673-1682

Authors:

D Sherrington, L Davison, A Buhot, JP Garrahan

Abstract:

We report a study of a series of simple model systems with only non-interacting Hamiltonians, and hence simple equilibrium thermodynamics, but with constrained dynamics of a type initially suggested by foams and idealized covalent glasses. We demonstrate that macroscopic dynamical features characteristic of real and more complex model glasses, such as two-time decays in energy and auto-correlation functions, arise from the dynamics and we explain them qualitatively and quantitatively in terms of annihilation-diffusion concepts and theory. The comparison is with strong glasses. We also consider fluctuation-dissipation relations and demonstrate subtleties of interpretation. We find no FDT breakdown when the correct normalization is chosen.