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Excited state structural analysis (ESSA) for correlated states of spin-flip type: application to electronic excitations in nanodiamonds with defects

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dc.contributor.author Luzanov, A.V.
dc.contributor.author Zhikol, O.A.
dc.date.accessioned 2017-06-12T11:03:11Z
dc.date.available 2017-06-12T11:03:11Z
dc.date.issued 2016
dc.identifier.citation Excited state structural analysis (ESSA) for correlated states of spin-flip type: application to electronic excitations in nanodiamonds with defects / A.V. Luzanov, O.A. Zhikol // Functional Materials. — 2016. — Т. 23, № 1. — С. 63-70. — Бібліогр.: 44 назв. — англ. uk_UA
dc.identifier.issn 1027-5495
dc.identifier.uri http://dspace.nbuv.gov.ua/handle/123456789/120559
dc.description.abstract The previously developed ESSA for configuration interaction singles (CIS) method is extended to a more rigorous many-body theory of excited states based on spin-flip (SF) transformations. The so-called SF-CIS (SF approach for CIS) is used, and the respective ESSA indices are constructed. These are atomic excitation indexes L*A, interatomic charge-transfer numbers lA - > B, and others. By using these quantities, low-lying excitations in the modelled nanodiamonds with color centers (first of all, nitrogen-vacancy (NV) centers) are investigated at a semiempirical level of the theory. It is shown that the lowest excitations are significantly localized in a vicinity of the vacancy. Furthermore, the same excitations are characterized by a high interatomic charge transfer. All these features are common to both types of the NV centers (neutral NV0 and negative NV-). uk_UA
dc.language.iso en uk_UA
dc.publisher НТК «Інститут монокристалів» НАН України uk_UA
dc.relation.ispartof Functional Materials
dc.subject Modeling and simulation uk_UA
dc.title Excited state structural analysis (ESSA) for correlated states of spin-flip type: application to electronic excitations in nanodiamonds with defects uk_UA
dc.type Article uk_UA
dc.status published earlier uk_UA
dc.identifier.udc :DOI: dx.doi.org/10.15407/fm23.01.063


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