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Electron-phonon coupling in d-electron solids: A temperature-dependent study of rutile TiO2 by first-principles theory and two-photon photoemission

MPG-Autoren
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Shang,  Honghui
NOMAD, Fritz Haber Institute, Max Planck Society;

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Carbogno,  Christian
NOMAD, Fritz Haber Institute, Max Planck Society;

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Scheffler,  Matthias
NOMAD, Fritz Haber Institute, Max Planck Society;

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PhysRevResearch.1.033153.pdf
(Verlagsversion), 990KB

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Zitation

Shang, H., Argondizzo, A., Tan, S., Zhao, J., Rinke, P., Carbogno, C., et al. (2019). Electron-phonon coupling in d-electron solids: A temperature-dependent study of rutile TiO2 by first-principles theory and two-photon photoemission. Physical Review Research, 1(3): 033153. doi:10.1103/PhysRevResearch.1.033153.


Zitierlink: https://hdl.handle.net/21.11116/0000-0005-62DC-5
Zusammenfassung
Rutile TiO2 is a paradigmatic transition-metal oxide with applications in optics, electronics, photocatalysis, etc., that are subject to pervasive electron-phonon interaction. To understand how energies of its electronic bands, and in general semiconductors or metals where the frontier orbitals have a strong d-band character, depend on temperature, we perform a comprehensive theoretical and experimental study of the effects of electron-phonon (e−p) interactions. In a two-photon photoemission (2PP) spectroscopy study we observe an unusual temperature dependence of electronic band energies within the conduction band of reduced rutile TiO2, which is contrary to the well-understood sp-band semiconductors and points to a so far unexplained dichotomy in how the e−p interactions affect differently the materials where the frontier orbitals are derived from the sp- and d orbitals. To develop a broadly applicable model, we employ state-of-the-art first-principles calculations that explain how phonons promote interactions between the Ti−3d orbitals of the conduction band within the octahedral crystal field. The characteristic difference in e−p interactions experienced by the Ti−3d orbitals of rutile TiO2 crystal lattice are contrasted with the more familiar behavior of the Si−2s orbitals of stishovite SiO2 polymorph, in which the frontier 2s orbital experiences a similar crystal field with the opposite effect. The findings of this analysis of how e−p interactions affect the d- and sp-orbital derived bands can be generally applied to related materials in a crystal field. The calculated temperature dependence of d-orbital derived band energies agrees well with and explains the temperature-dependent inter-d-band transitions recorded in 2PP spectroscopy of TiO2. The general understanding of how e−p interactions affect d-orbital derived bands is likely to impact the understanding of temperature-dependent properties of highly correlated materials.