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Spin-Wave Damping and Hydrodynamics in the Heisenberg Antiferromagnet
Author(s) -
A. B. Harris,
Deepak Kumar,
Bertrand I. Halperin,
P. C. Hohenberg
Publication year - 1970
Publication title -
journal of applied physics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.699
H-Index - 319
eISSN - 1089-7550
pISSN - 0021-8979
DOI - 10.1063/1.1658943
Subject(s) - spin wave , physics , isotropy , antiferromagnetism , condensed matter physics , anisotropy , spin (aerodynamics) , spin polarization , heisenberg model , curvature , quantum mechanics , thermodynamics , electron , geometry , mathematics , ferromagnetism
The Dyson‐Maleev formalism is used to calculate the decay rate of antiferromagnetic spin waves at low temperatures and long wavelengths. Various regimes must be distinguished depending on the relation between the wavevector k, the temperature T, and the anisotropy energy. For the isotropic system the relevant parameters are (a) the incident energy, (b) the thermal energy, (c) the deviation from linearity (``curvature energy'') of thermal spin waves, and (d) the curvature energy of the incident spin wave. In the anisotropic case the damping of the k=0 mode has the same dependence on spin‐wave energy as in the isotropic system. In all cases, the decay rate is small compared to the frequency, which implies that the spin waves are appropriate elementary excitations for small k and T, and that they interact weakly among themselves in this limit. For k→0 with T fixed, the decay rate is proportional to k2 in the isotropic system. This agrees with an earlier hydrodynamic prediction and contradicts previous micros...

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