view article
Figure 6
(a) Branching of the fundamental spectra σ(0) and σ(2) into [\sigma _{{a_{1g}}}^{\left(0 \right)}], [\sigma _{{e_g}}^{\left(0 \right)}] and [\sigma _{{t_{2g}}}^{\left(0 \right)}] of Fe3O4 using a cubic expansion. (b) Fe L2,3 XMLD with linear horizontal polarization (labelled LH) where the XMLD signal is defined as: XMLD = XAS(ϕ) − XAS(90°) and ϕ is the angle of the magnetic field. The measured (Exp.) and the calculated (Calc.) result from the cubic field expansion are shown in the left and right panels, respectively. (c) Fe L2,3 XMLD measured with linear polarization rotated 30° from the [1,0,0] (labelled L30) where the XMLD signal is defined as XMLD = XAS(ϕ) − XAS(60°).

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 28| Part 1| January 2021| Pages 247-258
https://doi.org/10.1107/S1600577520015027
Follow J. Synchrotron Rad.
Sign up for e-alerts
E-alerts
Follow J. Synchrotron Rad. on Twitter
Twitter
Follow us on facebook
Facebook
Sign up for RSS feeds
RSS