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Magnetic structure and magnon dynamics of the quasi-two-dimensional antiferromagnet<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msub><mml:mi>FePS</mml:mi><mml:mn>3</mml:mn></mml:msub></mml:math>

D. LançonEcole Polytechnique Fédérale de Lausanne, SB ICMP LQM, CH-1015 Lausanne, SwitzerlandH. C. WalkerISIS facility, Rutherford Appleton Laboratory, Harwell Oxford, Didcot OX11 0QX, UKE. RessoucheCEA-Grenoble/INAC, Laboratoire MDN, 17 rue des martyrs, 38054 Grenoble Cédex 9, FranceB. OuladdiafInstitut Laue-Langevin, CS 20156, 38042 Grenoble Cédex 9, FranceK. C. RuleAustralian Nuclear Science and Technology Organisation, Locked Bag 2001, Kirrawee DC NSW 2232, AustraliaGarry J. McIntyreAustralian Nuclear Science and Technology Organisation, Locked Bag 2001, Kirrawee DC NSW 2232, AustraliaT J HicksSchool of Physics, Monash University, Box 27, Clayton, Vic 3800, AustraliaH. M. RønnowEcole Polytechnique Fédérale de Lausanne, SB ICMP LQM, CH-1015 Lausanne, SwitzerlandAndrew WildesInstitut Laue-Langevin, CS 20156, 38042 Grenoble Cédex 9, France
2016lv
ABI

Аннотация

Neutron scattering from single crystals has been used to determine the magnetic structure and magnon dynamics of ${\text{FePS}}_{3}$, an $S=2$ Ising-like quasi-two-dimensional antiferromagnet with a honeycomb lattice. The magnetic structure has been confirmed to have a magnetic propagation vector of ${\mathbf{k}}_{M}=\left[01\frac{1}{2}\right]$ and the moments are collinear with the normal to the $ab$ planes. The magnon data could be modeled using a Heisenberg Hamiltonian with a single-ion anisotropy. Magnetic interactions up to the third in-plane nearest neighbor needed to be included for a suitable fit. The best fit parameters for the in-plane exchange interactions were ${J}_{1}=1.46, {J}_{2}=\ensuremath{-}0.04$, and ${J}_{3}=\ensuremath{-}0.96$ meV. The single-ion anisotropy is large, $\mathrm{\ensuremath{\Delta}}=2.66$ meV, explaining the Ising-like behavior of the magnetism in the compound. The interlayer exchange is very small, ${J}^{\ensuremath{'}}=\ensuremath{-}0.0073$ meV, proving that ${\text{FePS}}_{3}$ is a very good approximation to a two-dimensional magnet.

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