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Figure 2
Fine structure of the linear absorption coefficient of a Pt foil. The high-frequency oscillation dominating at energies lower than around 16 keV is the Pt L1 EXAFS contribution. Above 16 keV, the lower-frequency oscillation and the sharper structures are due to πXAFS (Nishino et al., 2000BB8).

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 8| Part 2| March 2001| Pages 105-109
doi:10.1107/S0909049501000590
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