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The potential calculations use the Hedin-Lundqvist (H-L) self-energy approximation. Trials with other approximation methods show no significant improvement. It is worth noting that an approximation formed by the Dirac-Fock self-energy for the core + H-L for valence electrons + a constant imaginary part leads to a very similar spectrum. Likewise, the use of a Dirac-Hara + imaginary part of the H-L potential induces a shift of 5 eV in the spectrum with respect to the edge, but without changing the shape of the spectrum
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The potential calculations use the Hedin-Lundqvist (H-L) self-energy approximation. Trials with other approximation methods show no significant improvement. It is worth noting that an approximation formed by the Dirac-Fock self-energy for the core + H-L for valence electrons + a constant imaginary part leads to a very similar spectrum. Likewise, the use of a Dirac-Hara + imaginary part of the H-L potential induces a shift of 5 eV in the spectrum with respect to the edge, but without changing the shape of the spectrum.
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