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Figure 1
XMCD spectra at the Ho L3 absorption edge (E0) of an HoFe2 sample obtained by switching the polarization helicity with a quarter-wave plate. (a) Spectrum obtained with a constant magnetic field parallel to the photon wavevector; (b) spectrum obtained with the magnetic field antiparallel to the photon wavevector; (c) pure XMCD signal without artifacts obtained as the half-difference of spectra (a) and (b); (d) pure residual spectrum R obtained as the half-sum of (a) and (b).

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 6| Part 6| November 1999| Pages 1125-1132
doi:10.1107/S0909049599011267
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