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Spin waves and the critical behaviour of the magnetization in

Andrew WildesClarendon Laboratory, University of Oxford, Parks Rd, Oxford, UKB. RoessliLaboratory for Neutron Scattering, ETH Zurich and Paul Scherrer Institute, 5232 Villigen, SwitzerlandB. LebechCondensed Matter Physics and Chemistry Department, Risø National Laboratory, DK-4000 Roskilde, DenmarkK. W. GodfreyClarendon Laboratory, University of Oxford, Parks Rd, Oxford, UK
1998en
ABI

Аннотация

Inelastic neutron scattering from a single crystal of the quasi-two-dimensional antiferromagnet MnPS<sub>3</sub> has been used to measure the spin wave dispersion curve at 4 K. The exchange integrals were subsequently calculated from linear spin wave theory. The values <em>J</em><sub>1</sub> = -0.77 meV, <em>J</em><sub>2</sub> = -0.07 meV, <em>J</em><sub>3</sub> = -0.18 meV and <em>J</em>′ = 0.0019 meV are within stability conditions calculated from mean-field theory. In addition, the critical behaviour of the gap in the spin wave energy at the Brillouin zone centre has been measured, and compared to the critical behaviour of the magnetization from neutron scattering data of the magnetic (020) Bragg peak. The gap varies with magnetization for <em>T</em> &lt; 0.96 <em>T<sub>N</sub></em>, and with the square of the magnetization for <em>T</em> &gt; 0.96 <em>T<sub>N</sub></em>. Two possible explanations are proposed: a competition between single-ion and dipolar anisotropies; or a crossover to <em>XY</em>-like excitations.

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