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Published on: December 4, 2014
Electronic structure study of YNbTiO[Formula: see text] and CaNb[Formula: see text]O[Formula: see text] with actinide
Daniil Maltsev1, Yuriy Lomachuk2, Vera Shakhova2
1Petersburg Nuclear Physics Institute named by B.P. Konstantinov of National Research Center "Kurchatov Institute" (NRC "Kurchatov Institute" - PNPI), mkr. Orlova roscha, 1, Leningrad district, 188300, Gatchina, Russian Federation. malcev_da@pnpi.nrcki.ru.
Abstract:
The compound-tunable embedding potential (CTEP) method is applied to study actinide substitutions in the niobate crystals YNbTiO[Formula: see text] and CaNb[Formula: see text]O[Formula: see text]. Two one-center clusters are built and centered on Y and Ca, and 20 substitutions of Y and Ca with U, Np, Pu, Am, and Cm were made in four different oxidation states for each cluster. Geometry relaxation is performed for each resulting structure, and electronic properties are analyzed by evaluating the spin density distribution and chemical shifts of X-ray emission spectra. Though the studied embedded clusters with actinides having the same oxidation state are found in general to yield similar local structure distortions, for Am, Cm and Pu in high "starting" oxidation states the electron transfer from the environment was found, resulting in decrease of their oxidation states. The U substitutions are additionally studied with the use of multi-center models, which can provide both more structural and electronic relaxation and also include charge-compensating vacancies. For "starting" U[Formula: see text] case, the decrease in the oxidation state similar to that of Am[Formula: see text] and Cm[Formula: see text] in one-center clusters is observed in our calculations but in a different way, while for "starting" U[Formula: see text] state the reverse process takes place, resulting in an increase in the oxidation state of uranium to U[Formula: see text]. It is known experimentally that the Nb and Ti atoms in YNbTiO[Formula: see text] are statistically distributed and occupy the same Wyckoff positions. With the CTEP method, it is possible to simulate to a certain extent the effects of such random distribution on the basis of perfect crystal calculation by performing Ti↔Nb substitutions in the embedded clusters. The results were compared to those obtained using the special quasirandom structures (SQS) method with structural relaxation for the single and double cell.
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