Thermodynamics of the one-dimensional half-filled Hubbard model in the spin-disordered regime

(2006)

Authors:

S Ejima, FHL Essler, F Gebhard

Artificial trapping of a stable high-density dipolar exciton fluid

(2006)

Authors:

Gang Chen, Ronen Rapaport, LN Pffeifer, K West, PM Platzman, Steven Simon, Z Voros, D Snoke

Drop dynamics on chemically patterned surfaces

(2006)

Authors:

H Kusumaatmaja, J Leopoldes, A Dupuis, JM Yeomans

Can nonlinear elasticity explain contact-line roughness at depinning?

Phys Rev Lett 96:1 (2006) 015702

Authors:

Pierre Le Doussal, Kay Jörg Wiese, Elie Raphael, Ramin Golestanian

Abstract:

We examine whether cubic nonlinearities, allowed by symmetry in the elastic energy of a contact line, may result in a different universality class at depinning. Standard linear elasticity predicts a roughness exponent zeta = 1/3 (one loop), zeta = 0.388 +/- 0.002 (numerics) while experiments give zeta approximately = 0.5. Within functional renormalization group methods we find that a nonlocal Kardar-Parisi-Zhang-type term is generated at depinning and grows under coarse graining. A fixed point with zeta approximately = 0.45 (one loop) is identified, showing that large enough cubic terms increase the roughness. This fixed point is unstable, revealing a rough strong-coupling phase. Experimental study of contact angles theta near pi/2, where cubic terms in the energy vanish, is suggested.

Commensurate and incommensurate ground states of Cs_2CuCl_4 in a magnetic field

ArXiv cond-mat/0601268 (2006)

Authors:

MY Veillette, JT Chalker

Abstract:

We present calculations of the magnetic ground state of Cs_2CuCl_4 in an applied magnetic field, with the aim of understanding the commensurately ordered state that has been discovered in recent experiments. This layered material is a realization of a Heisenberg antiferromagnet on an anisotropic triangular lattice. Its behavior in a magnetic field depends on field orientation, because of weak Dzyaloshinskii-Moriya interactions.We study the system by mapping the spin-1/2 Heisenberg Hamiltonian onto a Bose gas with hard core repulsion. This Bose gas is dilute, and calculations are controlled, close to the saturation field. We find a zero-temperature transition between incommensurate and commensurate phases as longitudinal field strength is varied, but only incommensurate order in a transverse field. Results for both field orientations are consistent with experiment.