X-ray absorption spectroscopy - fine edge structure

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SUMMARY

The fine edge structure in X-ray absorption spectroscopy (XAS) arises from the interactions of photoelectrons with neighboring atoms after they are ejected from the core shell. This phenomenon occurs just beyond the absorption edge, where the energy of incoming X-rays is sufficient to excite electrons. The scattering of these photoelectrons influences the absorption coefficient, leading to variations in the fine structure observed in XAS spectra. Understanding this relationship is crucial for interpreting XAS data accurately.

PREREQUISITES
  • X-ray absorption spectroscopy (XAS) fundamentals
  • Photoelectron scattering theory
  • Core shell electron excitation mechanisms
  • Absorption coefficient calculations
NEXT STEPS
  • Study the principles of X-ray absorption spectroscopy in detail
  • Explore the role of photoelectron scattering in material analysis
  • Investigate the mathematical models for calculating absorption coefficients
  • Examine case studies of fine edge structure in various materials
USEFUL FOR

Researchers in materials science, physicists studying electron interactions, and chemists utilizing X-ray absorption spectroscopy for material characterization will benefit from this discussion.

lavster
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Hi,

could someone tell me how the fine edge structure next the the absorbing edge in an XAS arises? from my understanding an XAS is a plot of absorption coefficient against energy of incoming xray. The absorption edge is at an energy corresponding to when the energy is just sufficient to excite an electron from the core shell to the vacuum. The fine edge structure is then somehting to do with the photoelectron wave but i didnt understand what i says in the literature...

Thanks
 
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Hi,

I guess it should be due to photoelectron, which leaves are scattered again by neighbouring atoms.
 
but why/how does this make any difference to the absorption coefficient of the material?!
 

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