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Electronic structure of hexagonal tungsten trioxide: XPS, XES, and XAS studies
X-Ray photoelectron (XPS), emission (XES) and absorption (XAS) spectroscopy methods were used to study the electronic structure of hexagonal tungsten trioxide, h-WO 3. Its precursor, hexagonal hydrogen tungsten bronze, H x WO 3, and the monoclinic form of tungsten trioxide, m-WO 3, were also studied...
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Published in: | Journal of alloys and compounds 2001-05, Vol.320 (1), p.1-6 |
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Main Authors: | , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | X-Ray photoelectron (XPS), emission (XES) and absorption (XAS) spectroscopy methods were used to study the electronic structure of hexagonal tungsten trioxide, h-WO
3. Its precursor, hexagonal hydrogen tungsten bronze, H
x
WO
3, and the monoclinic form of tungsten trioxide, m-WO
3, were also studied. For the mentioned compounds, both the XPS valence-band and core-level spectra, as well as the O Kα emission bands and the W L
III absorption edges were derived. It was established that, binding energies of both the W 4f and O 1s core-level electrons do not change when going from the tungsten trioxides to H
x
WO
3. A high-energy shift of the inflection point of the XAS W L
III spectrum of the H
x
WO
3 bronze, with respect to its position on the spectrum of pure metallic tungsten, was found to be close to those of the spectra of the two WO
3 forms studied. Half-widths of both the XPS valence-band spectra and the O Kα bands increase somewhat in the sequence m-WO
3→h-WO
3→H
x
WO
3. The formation of a near-Fermi sub-band, which is absent for both the modifications of WO
3, was observed on the XPS valence-band spectrum of hexagonal H
x
WO
3. The energy positions of the centers of gravity of the O Kα band remain constant for all the compounds studied. |
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ISSN: | 0925-8388 1873-4669 |
DOI: | 10.1016/S0925-8388(00)01454-7 |