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. Author manuscript; available in PMC: 2017 Jul 28.
Published in final edited form as: Phys Rev Lett. 2017 Mar 3;118(9):096402. doi: 10.1103/PhysRevLett.118.096402

FIG. 4.

FIG. 4

ΔSCF XAS rectified by the many-electron matrix formalism for TiO2 (a) and CrO2 (b). For comparison, the spectra produced by the one-body FCH formalism are denoted as 1p, and experimental (EXP) and BSE spectra as in Fig. 1 are also added with the first peaks aligned. (c) and (d) show the higher-order intensity contributions (in log scale) that do not exceed 0.004 in both cases.