2017
DOI: 10.1103/physrevb.95.155121
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Addressing electron-hole correlation in core excitations of solids: An all-electron many-body approach from first principles

Abstract: We present an ab initio study of core excitations of solid-state materials focusing on the role of electron-hole correlation. In the framework of an all-electron implementation of many-body perturbation theory into the exciting code, we investigate three different absorption edges of three materials, spanning a broad energy window, with transition energies between a few hundred to thousands of eV. Specifically, we consider excitations from the Ti K edge in rutile and anatase TiO2, from the Pb M4 edge in PbI2, … Show more

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Cited by 51 publications
(86 citation statements)
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References 67 publications
(95 reference statements)
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“…The experimental φ and θ angular evolution of the A2 amplitude (Figure 5b and 6a in the SI) matches a quadrupolar transition, qualitatively consistent with the dominant quadrupolar cross-section obtained from FDMNES calculations in the region of peak A2 ( Figure 2b, inset and Figure 3b). Recent calculations accounting for the electron-hole interaction in the Bethe-Salpeter equation have reproduced peak A2, although with an underestimated amplitude as in our FDM calculations [31]. Peaks A1 and A2 are found to exhibit their maximum amplitude when the electric field is parallel to the (a, b) and c axes, respectively.…”
Section: B Origin Of Peak A2supporting
confidence: 65%
See 1 more Smart Citation
“…The experimental φ and θ angular evolution of the A2 amplitude (Figure 5b and 6a in the SI) matches a quadrupolar transition, qualitatively consistent with the dominant quadrupolar cross-section obtained from FDMNES calculations in the region of peak A2 ( Figure 2b, inset and Figure 3b). Recent calculations accounting for the electron-hole interaction in the Bethe-Salpeter equation have reproduced peak A2, although with an underestimated amplitude as in our FDM calculations [31]. Peaks A1 and A2 are found to exhibit their maximum amplitude when the electric field is parallel to the (a, b) and c axes, respectively.…”
Section: B Origin Of Peak A2supporting
confidence: 65%
“…This explains the relatively intense A2 peak in amorphous TiO 2 [24] or upon electron trapping at defects after photoexcitation of anatase or rutile TiO 2 [25,26,29]. The unprecedented quantitative agreement provided in this work is made possible by the continued improvement of computational codes including full potentials [18][19][20] and the more accurate description of the core-hole interaction in Bethe-Salpeter calculations [31,55]. Experiments are on-going to extend this work to rutile TiO 2 .…”
Section: Discussionmentioning
confidence: 66%
“…The adopted theoretical formalism, based on all-electron DFT 25 , allows to access the energies of all the electrons in the core. Although core energies are systematically underestimated by 10–20% in DFT 26 , relative core shifts referred to the same levels in different materials can be correlated with XPS data in a meaningful way. The calculated core level energies of each state in all the investigated materials are reported in Table 2.…”
Section: Resultsmentioning
confidence: 99%
“…In fact, recent ab initio studies using the Green's function approach showed the accurate prediction of core electron binding energy in XPS simulations [34][35][36] . Especially, the GW+Bethe-Salpeter equation (GW + BSE) method has been widely used for simulating the XAS spectra in molecule, cluster, and solid systems [37][38][39][40] . The success of the Green's-function approach in XPS and XAS simulations results from the accurate descriprtion of the screening ef-fect due to the core hole state within the GW approximation (GWA) [41][42][43][44] .…”
Section: Introductionmentioning
confidence: 99%