Book contents
- Frontmatter
- Contents
- Preface
- 1 Introduction
- 2 Basic physics of X-ray absorption and scattering
- 3 Experimental
- 4 Theory
- 5 Data analysis
- 6 Related techniques and conclusion
- Appendix 1 Introduction to Fourier transforms in EXAFS
- Appendix 2 Cumulants in EXAFS
- Appendix 3 Optimizing X-ray filters
- Appendix 4 Reference spectra
- Appendix 5 X-ray tables
- References
- Index
1 - Introduction
Published online by Cambridge University Press: 25 January 2011
- Frontmatter
- Contents
- Preface
- 1 Introduction
- 2 Basic physics of X-ray absorption and scattering
- 3 Experimental
- 4 Theory
- 5 Data analysis
- 6 Related techniques and conclusion
- Appendix 1 Introduction to Fourier transforms in EXAFS
- Appendix 2 Cumulants in EXAFS
- Appendix 3 Optimizing X-ray filters
- Appendix 4 Reference spectra
- Appendix 5 X-ray tables
- References
- Index
Summary
What is XAFS?
X-ray Absorption Fine Structure (XAFS) spectroscopy is a unique tool for studying, at the atomic and molecular scale, the local structure around selected elements that are contained within a material. XAFS can be applied not only to crystals, but also to materials that possess little or no long-range translational order: amorphous systems, glasses, quasicrystals, disordered films, membranes, solutions, liquids, metalloproteins – even molecular gases. This versatility allows it to be used in a wide variety of disciplines: physics, chemistry, biology, biophysics, medicine, engineering, environmental science, materials science, and geology.
The basic physical quantity that is measured in XAFS is the X-ray absorption coefficient µ(E), which describes how strongly X-rays are absorbed as a function of X-ray energy E. Generally µ(E) smoothly decreases as the energy increases (approximately as 1/E3), i.e. the X-rays become more penetrating. However, at specific energies that are characteristic of the atoms in the material, there are sudden increases called X-ray absorption edges. These occur when the X-ray photon has sufficient energy to liberate electrons from the low-energy bound states in the atoms. The cross section, a quantity that is proportional to µ(E), is shown in Figure 1.1 for the element platinum. Experimental data for MnO and KMnO4 are shown in Figures 1.2 and 1.3.
Absorption edges were first measured in 1913 by Maurice De Broglie, the older brother of quantum mechanics pioneer Louis De Broglie.
- Type
- Chapter
- Information
- Introduction to XAFSA Practical Guide to X-ray Absorption Fine Structure Spectroscopy, pp. 1 - 7Publisher: Cambridge University PressPrint publication year: 2010
- 1
- Cited by