Two-magnon excitations observed by neutron scattering in the two-dimensional spin-5/2 Heisenberg antiferromagnet Rb2MnF4

(2005)

Authors:

T Huberman, R Coldea, RA Cowley, DA Tennant, RL Leheny, RJ Christianson, CD Frost

Two-magnon excitations observed by neutron scattering in the two-dimensional spin-5/2 Heisenberg antiferromagnet Rb2MnF4

ArXiv cond-mat/0504684 (2005)

Authors:

T Huberman, R Coldea, RA Cowley, DA Tennant, RL Leheny, RJ Christianson, CD Frost

Abstract:

The low-temperature magnetic excitations of the two-dimensional spin-5/2 square-lattice Heisenberg antiferromagnet Rb2MnF4 have been probed using pulsed inelastic neutron scattering. In addition to dominant sharp peaks identified with one-magnon excitations, a relatively weak continuum scattering is also observed at higher energies. This is attributed to neutron scattering by pairs of magnons and the observed intensities are consistent with predictions of spin wave theory.

Three-dimensional spin fluctuations in Na0.75CoO2

Physical Review Letters 94 (2005) article 157206 4pp

Authors:

LM Helme, AT Boothroyd, R Coldea, D Prabhakaran, DA Tennant, A Hiess, J Kulda

Ground states of a frustrated spin-1/2 antifferomagnet: Cs_2CuCl_4 in a magnetic field

(2005)

Authors:

MY Veillette, JT Chalker, R Coldea

Ground states of a frustrated spin-1/2 antifferomagnet: Cs_2CuCl_4 in a magnetic field

ArXiv cond-mat/0501347 (2005)

Authors:

MY Veillette, JT Chalker, R Coldea

Abstract:

We present detailed calculations of the magnetic ground state properties of Cs$_2$CuCl$_4$ in an applied magnetic field, and compare our results with recent experiments. The material is described by a spin Hamiltonian, determined with precision in high field measurements, in which the main interaction is antiferromagnetic Heisenberg exchange between neighboring spins on an anisotropic triangular lattice. An additional, weak Dzyaloshinkii-Moriya interaction introduces easy-plane anisotropy, so that behavior is different for transverse and longitudinal field directions. We determine the phase diagram as a function of field strength for both field directions at zero temperature, using a classical approximation as a first step. Building on this, we calculate the effect of quantum fluctuations on the ordering wavevector and components of the ordered moments, using both linear spinwave theory and a mapping to a Bose gas which gives exact results when the magnetization is almost saturated. Many aspects of the experimental data are well accounted for by this approach.