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Figure 7
The time-evolution of the Gd L3-edge XMCD amplitude of GdCo3 (circles and squares) is compared with the field pulse (full lines) for two intensities of the field pulse (0.3 and 0.7 T). In the inset the amplitude of the XMCD signal obtained with a static field from −1 T to 1 T is shown.

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 5| Part 5| September 1998| Pages 1298-1303
https://doi.org/10.1107/S0909049598004154
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