2009
DOI: 10.1103/physrevb.79.041102
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All-electron Bethe-Salpeter calculations for shallow-core x-ray absorption near-edge structures

Abstract: X-ray absorption near-edge structure spectra are calculated by fully solving the electron/core-hole Bethe-Salpeter equation ͑BSE͒ in an all-electron framework. We study transitions from shallow core states, including the Mg L 2,3 edge in MgO, the Li K edge in the Li halides LiF, LiCl, LiBr, and LiI, as well as Li 2 O. We illustrate the advantage of the many-body approach over a core-hole supercell calculation. Both schemes lead to strongly bound excitons, but the nonlocal treatment of the electron-hole interac… Show more

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Cited by 73 publications
(73 citation statements)
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“…The theoretical problems with the leading peaks (B, B2) are likely related to the frozen-core approximation and to dynamical screening effects, i.e., the energy dependence of the complex self-energy [31,32]. The nonlocality of the particle-hole exchange interaction [33] is a further issue. It should be noted that the poor descrip- tion of the leading peaks is a common problem for K-edge XANES of light elements and could so far not be cured by any ab initio method we are aware of, including the Bethe-Salpeter-Equation approach [34].…”
Section: Xanes Of Graphenementioning
confidence: 99%
“…The theoretical problems with the leading peaks (B, B2) are likely related to the frozen-core approximation and to dynamical screening effects, i.e., the energy dependence of the complex self-energy [31,32]. The nonlocality of the particle-hole exchange interaction [33] is a further issue. It should be noted that the poor descrip- tion of the leading peaks is a common problem for K-edge XANES of light elements and could so far not be cured by any ab initio method we are aware of, including the Bethe-Salpeter-Equation approach [34].…”
Section: Xanes Of Graphenementioning
confidence: 99%
“…With the core-hole potential directly included in the calculation of the electronic states, this method is well suited for extended systems [14][15][16], although requiring supercell calculations to avoid spurious interactions between core holes of neighboring unit cells. For shallower core states, however, the overlap between the initial core state and the conduction bands * vorwerk@physik.hu-berlin.de is usually more relevant and the local treatment of the electron-hole correlation becomes problematic [17]. Indeed, the core-hole approximation is known to fail in case of excitations involving shallow core or even semi-core states, that may interact with the surrounding electrons [18].…”
Section: Introductionmentioning
confidence: 99%
“…3c), is confined within the layer of the absorbing atom. Its extension beyond the size of the unit cell of the material is a signature of the electron-hole correlation, which is typical of bound excitons in the core [17,18,23,56], as well as in the valence region (see, e.g., [8,57]). It is worth noting that the first core exciton in PbI 2 is much more localized than its counterpart in the optical region [55].…”
Section: B Lead M4-edge Spectrum Of Pbi2mentioning
confidence: 99%
“…On the other hand, this method is known to perform worse for excitations from shallow core or semicore states, where e-h correlation becomes relevant [29][30][31][32]. In the core-hole approximation, the exciton binding strength relies on the adopted approximation for the exchange-correlation functional [33]. Moreover, this method requires the construction of a supercell to avoid spurious interactions between neighboring coreholes.…”
Section: B Theoretical Backgroundmentioning
confidence: 99%