XPS spectra of uranyl minerals and synthetic uranyl compounds. II: The O 1s spectrum
The O 1s spectrum is examined for 19 uranyl minerals of different composition and structure. Spectra from single crystals were measured with a Kratos Axis Ultra X-ray Photoelectron Spectrometer with a magnetic-confinement charge-compensation system. Well-resolved spectra with distinct maxima, should...
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Veröffentlicht in: | Geochimica et cosmochimica acta 2009-05, Vol.73 (9), p.2488-2509 |
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Sprache: | eng |
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Zusammenfassung: | The O 1s spectrum is examined for 19 uranyl minerals of different composition and structure. Spectra from single crystals were measured with a Kratos Axis Ultra X-ray Photoelectron Spectrometer with a magnetic-confinement charge-compensation system. Well-resolved spectra with distinct maxima, shoulders and inflections points, in combination with reported and measured binding energies for specific O
2− species and structural data of the uranyl minerals are used to resolve the fine structure of the O 1s envelope. The resolution of the O 1s spectra includes, for the first time, different O
2− bands, which are assigned to O atoms linking uranyl with uranyl polyhedra (
U
O
U) and O atoms of uranyl groups (
O
U
O). The resolved bands in the O 1s spectrum occur at distinct ranges in binding energy: bands for (
U
O
U) occur at 529.6–530.4
eV, bands for (
O
U
O) occur at 530.6–531.4
eV, bands for O
2− in the equatorial plane of the uranyl polyhedra linking uranyl polyhedra with (
TO
n
) groups (
T
=
Si, S, C, P, Se) (
T
O) occur at 530.9–532.2
eV; bands for (OH) groups in the equatorial plane of the uranyl polyhedra (
OH) occur at 532.0–532.5
eV, bands of (H
2O) groups in the interstitial complex of the uranyl minerals (
H
2
O
interst
) occur at 533.0–533.8
eV and bands of physisorbed (H
2O) groups on the surface of uranyl minerals (
H
2
O
adsorb
) occur at 534.8–535.2
eV. Treatment of uranyl minerals with acidic solutions results in a decrease in
U
O
U and an increase in
OH. Differences in the ratio of
OH
:
O
U
O between the surface and bulk structure is larger for uranyl minerals with a high number of
U
O
U and
T
O species in the bulk structure which is explained by protonation of underbonded
U
O,
U
O
U and
T
O terminations on the surface. The difference in the ratio of
H
2
O
interst
:
O
U
O between the bulk and surface structures is larger for uranyl minerals with higher percentages of
H
2
O
interst
as well as, with a higher number of interstitial H
2O groups that are not bonded to interstitial cations, resulting in easier dehydration of interstitial H
2O groups in uranyl minerals during exposure to a vacuum. |
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ISSN: | 0016-7037 1872-9533 |
DOI: | 10.1016/j.gca.2008.10.041 |