Linear dichroic x-ray absorption response of Ti-Ti dimers along the \(c\) axis in Ti\(_2\)O\(_3\) upon Mg substitution
Corundum oxide Ti\(_2\)O\(_3\) shows the metal-insulator transition around 400-600 K accompanying the nearest Ti\(^{3+}\)-Ti\(^{3+}\) bond (\(a_{1g}a_{1g}\) singlet state) formation along the \(c\) axis. In order to clarify the hole-doping effect for the \(a_{1g}a_{1g}\) singlet bond in Ti\(_2\)O\(_...
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Veröffentlicht in: | arXiv.org 2023-11 |
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Sprache: | eng |
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Zusammenfassung: | Corundum oxide Ti\(_2\)O\(_3\) shows the metal-insulator transition around 400-600 K accompanying the nearest Ti\(^{3+}\)-Ti\(^{3+}\) bond (\(a_{1g}a_{1g}\) singlet state) formation along the \(c\) axis. In order to clarify the hole-doping effect for the \(a_{1g}a_{1g}\) singlet bond in Ti\(_2\)O\(_3\), we investigated Ti \(3d\) orbital anisotropy between corundum-type Ti\(_2\)O\(_3\) and ilmenite-type MgTiO\(_3\) using linear dichroism of soft x-ray absorption spectroscopy of the Ti \(L_{2,3}\) edge. From the linear dichroic spectral weight in Mg\(_y\)Ti\(_{2-y}\)O\(_3\), we confirmed that the \(a_{1g}a_{1g}\) state is dominant not only in \(y=0.01\) (almost Ti\(_2\)O\(_3\)), but also in \(y = 0.29\), indicating that the Ti-Ti bond survives against a certain level of hole doping. In \(y=0.63\) corresponding to 46% hole doping per Ti, the \(3d\) orbital symmetry changes from \(a_{1g}\) to \(e_g^{\pi}\). |
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ISSN: | 2331-8422 |
DOI: | 10.48550/arxiv.2311.04814 |