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Resonant and Non-resonant Phenomena in RIXS

Resonant and Non-resonant Phenomena in RIXS. Spectroscopic aspects of RIXS Resonant and non-resonant Integrated 2p3d RIXS (FY detection) Removing the obscuring silent majority. resonant inelastic x-ray scattering/spectroscopy. 2p XAS: 2p3d integrals & 2p spin-orbit coupling. 3d.

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Resonant and Non-resonant Phenomena in RIXS

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  1. Resonant and Non-resonant Phenomena in RIXS • Spectroscopic aspects of RIXS • Resonant and non-resonant • Integrated 2p3d RIXS (FY detection) • Removing the obscuring silent majority

  2. resonant inelastic x-ray scattering/spectroscopy

  3. 2p XAS: 2p3d integrals & 2p spin-orbit coupling 3d <2p3d|1/r|2p3d> 2p3/2 2p1/2 Phys. Rev. B. 42, 5459 (1990)

  4. CTM4XAS (semi-empirical)

  5. 2p3s RIXS of CaF2 3d0 → 2p5 3d1 → 3s1 3d1 Rubensson et al. Phys. Rev. B. 49, 1507 (1994); Phys. Rev. B. 53, 7099 (1996)

  6. 2p3s RIXS of CaF2 Is interference important? If not RIXS = XAS * XES Rubensson et al. Phys. Rev. B. 49, 1507 (1994); Phys. Rev. B. 53, 7099 (1996)

  7. 2p3s RIXS of CaF2 Is interference important? If not RIXS = XAS * XES Rubensson et al. Phys. Rev. B. 49, 1507 (1994); Phys. Rev. B. 53, 7099 (1996)

  8. La 4d5p RIXS: importance of interference 4f0 4d9 4f1[3D1]  5p1 4f1 Phys. Rev. Lett. 103, 137401 (2009)

  9. La 4d5p RIXS: importance of interference 4f0 4d9 4f1[3D1]  5p1 4f1 Resonant XES spectra change within a single resonance Phys. Rev. Lett. 103, 137401 (2009)

  10. La 4d5p RIXS: importance of interference 3D1 pre-edge interferes with tail of delayed onset at 17 eV Phys. Rev. Lett. 103, 137401 (2009)

  11. 2p3s RIXS of CaF2 3d0 → 2p5 3d1 → 3s1 3d1 Rubensson et al. Phys. Rev. B. 49, 1507 (1994); Phys. Rev. B. 53, 7099 (1996)

  12. Resonant and non-resonant XAS * XES XPS * XES Phys. Rev. B. 53, 7099 (1996)

  13. Resonant and non-resonant XPS * XES Glatzel et al., Phys. Rev. B. 64, 045109 (2001)

  14. Resonant and non-resonant XAS * XES XPS * XES Phys. Rev. B. 53, 7099 (1996)

  15. ‘non-resonant peak’ only visible at resonance Ground state: 3d8 + 3d9 + 3d10 XAS main: 3d9 XAS CT: 3d10 XPS: <1% 3d10 Finazzi et al. PRB 59, 9933 (1999)

  16. 2p3d RIXS of NiO S MS dd ‘spin-flip’ spin-flip Phys. Rev. B. 57, 14584 (1998)

  17. 2p3d RIXS XES of CoO Van Schooneveld et al. J. Phys. Chem. C. 116, 15218 (2012)

  18. CTM4RIXS (semi-empirical) (crystal fields, exchange field, spin-orbit, [charge transfer]) CTM4RIXS by P. Glatzel, E. Stavitski et al.

  19. Fluorescence Yield = integrated 2p3d RIXS • FY-XAS ≠ XAS • L2 edge increases & High-energies increase • Sum rules break down • Strong polarization dependence Kurian J. Phys. Cond. Matt. 24, 435602 (2012)

  20. Dips and peaks in FY-XAS Nature Chem. 4, 766 (2012)

  21. Problem: XAS measures average of all atoms

  22. Nanoscale chemical imaging of a working catalyst Carbon K-edge 1 bar, 350 C de Smit et al. Nature 456, 222 (2008); Angew. Chem. 48, 3632 (2009)

  23. Problem: XAS measures average of all atoms • 2p XAS under in-situ conditions • Measure different valences in one spectrum • GOAL: measure spectra for each valence separate

  24. Valence selective XAS Glatzel et al. Inorg. Chem. 41, 3121 (2002)

  25. Removing the silent majority 2p XAS of Co2+ and Co3+

  26. Removing the silent majority 2p XAS of Co2+ and Co3+

  27. Removing the silent majority 2p RIXS of Co2+ and Co3+

  28. Removing the silent majority 2p RIXS of Co2+ and Co3+

  29. Acknowledgements Utrecht University:Matti van Schooneveld (Mülheim) Reshmi Kurian Piter Miedema (Bessy) Emiel de Smit (Exxon) Fernando Morales (Topsoe) Eli Stavitski (CLS) Thorsten Schmidt (SLS) Pieter Glatzel (ESRF)

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