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. 2017 Oct 17;7(1):13317.
doi: 10.1038/s41598-017-13607-6.

Cationic double K-hole pre-edge states of CS2 and SF6

Affiliations

Cationic double K-hole pre-edge states of CS2 and SF6

R Feifel et al. Sci Rep. .

Abstract

Recent advances in X-ray instrumentation have made it possible to measure the spectra of an essentially unexplored class of electronic states associated with double inner-shell vacancies. Using the technique of single electron spectroscopy, spectra of states in CS2 and SF6 with a double hole in the K-shell and one electron exited to a normally unoccupied orbital have been obtained. The spectra are interpreted with the aid of a high-level theoretical model giving excellent agreement with the experiment. The results shed new light on the important distinction between direct and conjugate shake-up in a molecular context. In particular, systematic similarities and differences between pre-edge states near single core holes investigated in X-ray absorption spectra and the corresponding states near double core holes studied here are brought out.

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Conflict of interest statement

The authors declare that they have no competing interests.

Figures

Figure 1
Figure 1
Schematic illustration of the two channels contributing to single photon K −2 V processes. The red (green) arrows represent the direct (conjugate) path. The curved arrows correspond to photo-excitation processes. The straight arrows correspond to shake processes.
Figure 2
Figure 2
Experimental (lower panel) and theoretical (upper panel) K −2 V spectrum of C*S2. The theoretical spectrum is based on DFT/B3LYP binding energies (see Table 1). The main peaks are illustrated by electronic iso-density plots. Red lines: direct contributions; green lines: conjugate contributions; black curve: incoherent sum of direct and conjugate contributions.
Figure 3
Figure 3
Experimental sulphur K −2 V spectrum of CS2.
Figure 4
Figure 4
Experimental (lower panel) and theoretical (upper panel) sulphur K −2 V spectra of SF6. Red lines reflect the direct contributions and green lines reflect conjugate contributions. The black curve represents an incoherent sum of the direct and conjugate contributions.
Figure 5
Figure 5
Experimental (lower panel) and theoretical (upper panel) K −2 V spectra of SF6. The position of the theoretical low-lying band is set to 1476.04 eV (see Table 1, HF-MP2).

References

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