2016
DOI: 10.1080/00150193.2016.1198196
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On the nature of change in Ni oxidation state in BaTiO3–SrTiO3system

Abstract: XAFS studies of Ni-doped Ba1−xSrxTiO3 solid solution reveal that the Ni oxidation state changes from 4 in SrTiO3 to 2.5 in BaTiO3 when varying x. This change is accompanied by a noticeable change in the interatomic Ni-O distances in the first shell. The first-principles calculations show that nickel creates an impurity band in the forbidden band gap of BaTiO3 and SrTiO3, which explains the appearance of intense absorption of Ni-doped samples in the visible region. The analysis of the electronic structure of do… Show more

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Cited by 15 publications
(11 citation statements)
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“…More recent work on Ni-doped hexagonal BaTiO 3 ceramics confirmed the majority of defects to be Ni 2? as determined by x-ray photoelectron spectroscopy (XPS) [10,26] or to be a mixture between Ni 2? and small amounts of Ni 3? as derived from extended x-ray absorption fine structure (EXAFS) measurements [27]. In the latter paper, the presence of the charge-compensating oxygen vacancy in the first coordination sphere of the Ni defect was excluded.…”
Section: Introductionmentioning
confidence: 99%
“…More recent work on Ni-doped hexagonal BaTiO 3 ceramics confirmed the majority of defects to be Ni 2? as determined by x-ray photoelectron spectroscopy (XPS) [10,26] or to be a mixture between Ni 2? and small amounts of Ni 3? as derived from extended x-ray absorption fine structure (EXAFS) measurements [27]. In the latter paper, the presence of the charge-compensating oxygen vacancy in the first coordination sphere of the Ni defect was excluded.…”
Section: Introductionmentioning
confidence: 99%
“…Therefore, the grain boundary segregation and dissolution of cations determine the grain boundary resistance. Ni is known as an acceptor-type dopant for BT and it readily dissolves into Ti sites by introducing oxygen vacancies in BT [23]. Oxygen vacancies are one of the major causes for IR degradation during constant poling with a DC bias [8].…”
Section: Resultsmentioning
confidence: 99%
“…Параметры, описывающие кулоновское и обменное взаимодействие для примесного атома, полагались равными U = 5 eV и J = 0.9 eV. Как было показано в наших более ранних исследованиях [35], чтобы получить относительно узкие примесные полосы в энергетическом спектре, необходимо использовать сверхъячейки, содержащие более 40 атомов. Поэтому для моделирования изолированных примесных центров нами использовались 80-атомные ГЦК-сверхъячейки, в которых один из ионов Ti 4+ в узле B или ионов Sr 2+ в узле A замещался атомом примеси.…”
Section: эксперимент и техника расчетовunclassified