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Figure 1
(a) Schematic of the scattering geometry. (b) Fe L2,3 XAS measurements in Fe3O4 with four linearly independent incident polarizations as described in Table 1[link] with the magnetic field (B) kept parallel to [1,0,0]. (c) The real part of the response function computed by applying a Kramers–Kronig transformation on the XAS measurements in (b). (d) Matrix elements of the conductivity tensor created from linear combinations of the experimental measurements while the XMLD and XMCD measurements are shown in panels (e) and (f), respectively.

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 28| Part 1| January 2021| Pages 247-258
https://doi.org/10.1107/S1600577520015027
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