The magnetic excitation spectra of Gd were measured by neutron inelastic scattering over the entire Brillouin zone in the 〈110〉 direction at temperatures from 250 to 850 K (Tc=293 K). The data were fitted to a damped-harmonic-oscillator form for the spectral weight function and were placed on an absolute cross-section basis. Wave-vector-dependent susceptibilities were obtained by integration over energy. They clearly show the presence of static spin correlations even at T=850 K. At T{≥}Tc we observe a crossover from spin-diffusive motion at small q to spin-wave behavior at large q. The wave vector qc at which this crossover occurs is determined by the ratio of the damping parameter to the second moment, 〈ω²〉, of the frequency distribution. Surprisingly, 〈ω²〉 remains independent of temperature above Tc, and the temperature dependence of qc is therefore determined by a gradual change in the damping. This results in a very weak qc-versus-T dependence, which is not consistent with a magnetic short-range-order interpretation for the existence of spin waves above Tc.
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Cable et al. (1989) studied this question.
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