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Figure 5
(a) The field dependence of the magnetic distance distribution function Pmag(r) at 280 K. The Pmag(r) values were computed numerically via an indirect Fourier transform (IFT) of the experimental dΣmag/dΩ data shown in Fig. 4[link](b). Note that for comparison with the results obtained at lower temperatures, as summarized in Appendix C[link], the Pmag at each field has been normalized by the maximum peak intensity value obtained at remanence. (Inset) A comparison between the experimental dΣmag/dΩ plotted in Fig. 4[link](b) (coloured open circles) and the reconstructed dΣmag/dΩ based on the IFT of the numerically computed Pmag shown in Fig. 5(a) (coloured solid lines). (b) The corresponding magnetic correlation function Cmag(r) = Pmag(r)/r2 (semi-logarithmic sale).

Journal logoJOURNAL OF
APPLIED
CRYSTALLOGRAPHY
ISSN: 1600-5767
Volume 55| Part 4| August 2022| Pages 713-721
https://doi.org/10.1107/S1600576722006355
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