Open AccessDevelopment of XAFS theory
Author(s) -
Ankudinov A. L.,
Rehr J. J.
Publication year - 2003
Publication title -
journal of synchrotron radiation
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.172
H-Index - 99
ISSN - 1600-5775
DOI - 10.1107/s0909049503009130
Subject(s) - xanes , x ray absorption fine structure , extended x ray absorption fine structure , electronic structure , physics , absorption (acoustics) , atomic physics , field (mathematics) , atom (system on chip) , scattering , electron , ab initio , density functional theory , chemistry , absorption spectroscopy , condensed matter physics , spectral line , quantum mechanics , spectroscopy , optics , mathematics , computer science , pure mathematics , embedded system
A major goal of theoretical simulations of X‐ray absorption fine structure (XAFS) is to provide calculations for the interpretation and analysis of experimental data in terms of geometrical and electronic information. The extended region or EXAFS (50–2000 eV above an absorption edge) contains geometric information about the pair distribution function, i.e. distances to the nearest neighbors and their orientation. The theory of EXAFS is now well understood and has been recently reviewed [Rehr & Albers (2000). Rev. Mod. Phys. 72 , 621–654]. The near‐edge region (0–50 eV above the edge) or X‐ray absorption near‐edge structure (XANES) probes the states just above the Fermi level, and contains important electronic information, e.g. the electronic density of states (DOS). This data can be used to obtain the number of electrons or holes in the electronic configuration and spin and orbital moments on a particular atom via sum rules. XANES calculations with our ab initio code FEFF8 [Ankudinov et al. (1998). Phys. Rev. B , 58 , 7565–7576] usually give semi‐quantitative agreement with experiment, and permits the interpretation of XANES in terms of DOS. However, fully quantitative calculations remain a challenge. Several effects still need to be considered to treat the XANES region. These include non‐spherical parts of the scattering potential and many‐body effects such as multi‐electron excitations, core‐hole effects and local field effects (screening of the X‐ray field).