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XPS spectra of uranyl minerals and synthetic uranyl compounds. II: The O 1s spectrum
Authors:M Schindler  FC Hawthorne  PC Burns
Institution:a Department of Geological Sciences, University of Manitoba, Winnipeg, Man., Canada R3T2N2
b Department of Chemistry, University of Manitoba, Winnipeg, Man., Canada R3T2N2
c Department of Civil Engineering and Geological Sciences, University of Notre Dame, IN 46556-0767, USA
Abstract: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 O2− 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 O2− bands, which are assigned to O atoms linking uranyl with uranyl polyhedra (Usingle bondOsingle bondU) and O atoms of uranyl groups (Odouble bond; length as m-dashUdouble bond; length as m-dashO). The resolved bands in the O 1s spectrum occur at distinct ranges in binding energy: bands for (Usingle bondOsingle bondU) occur at 529.6-530.4 eV, bands for (Odouble bond; length as m-dashUdouble bond; length as m-dashO) occur at 530.6-531.4 eV, bands for O2− in the equatorial plane of the uranyl polyhedra linking uranyl polyhedra with (TOn) groups (T = Si, S, C, P, Se) (Tsingle bondO) 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 (H2O) groups in the interstitial complex of the uranyl minerals (H2Ointerst) occur at 533.0-533.8 eV and bands of physisorbed (H2O) groups on the surface of uranyl minerals (H2Oadsorb) occur at 534.8-535.2 eV. Treatment of uranyl minerals with acidic solutions results in a decrease in Usingle bondOsingle bondU and an increase in OH. Differences in the ratio of OH Odouble bond; length as m-dashUdouble bond; length as m-dashO between the surface and bulk structure is larger for uranyl minerals with a high number of Usingle bondOsingle bondU and Tsingle bondO species in the bulk structure which is explained by protonation of underbonded Usingle bondO, Usingle bondOsingle bondU and Tsingle bondO terminations on the surface. The difference in the ratio of H2Ointerst Odouble bond; length as m-dashUdouble bond; length as m-dashO between the bulk and surface structures is larger for uranyl minerals with higher percentages of H2Ointerst as well as, with a higher number of interstitial H2O groups that are not bonded to interstitial cations, resulting in easier dehydration of interstitial H2O groups in uranyl minerals during exposure to a vacuum.
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