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dc.contributor.authorPotashnikov, S. I.en
dc.contributor.authorBoyarchenkov, A. S.en
dc.contributor.authorNekrasov, K. A.en
dc.contributor.authorKupryazhkin, A. Y.en
dc.date.accessioned2014-11-29T19:45:52Z-
dc.date.available2014-11-29T19:45:52Z-
dc.date.issued2013-
dc.identifier.citationHigh-precision molecular dynamics simulation of UO2-PuO 2: Anion self-diffusion in UO2 / S. I. Potashnikov, A. S. Boyarchenkov, K. A. Nekrasov [et al.] // Journal of Nuclear Materials. — 2013. — Vol. 433. — № 1-3. — P. 215-226.en
dc.identifier.issn0022-3115-
dc.identifier.other1good_DOI
dc.identifier.other46529f88-1636-4da6-9d7c-cdc433f372d0pure_uuid
dc.identifier.otherhttp://www.scopus.com/inward/record.url?partnerID=8YFLogxK&scp=84867895212m
dc.identifier.urihttp://elar.urfu.ru/handle/10995/27142-
dc.description.abstractOur series of articles is devoted to high-precision molecular dynamics simulation of mixed actinide-oxide (MOX) fuel in the approximation of rigid ions and pair interactions (RIPI) using high-performance graphics processors (GPU). In this article we study self-diffusion mechanisms of oxygen anions in uranium dioxide (UO2) with the 10 recent and widely used sets of interatomic pair potentials (SPP) under periodic (PBC) and isolated (IBC) boundary conditions. Wide range of measured diffusion coefficients (from 10-3 cm2/s at melting point down to 10-12 cm2/s at 1400 K) made possible a direct comparison (without extrapolation) of the simulation results with the experimental data, which have been known only at low temperatures (T < 1500 K). A highly detailed (with the temperature step of 1 K) calculation of the diffusion coefficient allowed us to plot temperature dependences of the diffusion activation energy and its derivative, both of which show a wide (∼1000 K) superionic transition region confirming the broad λ-peaks of heat capacity obtained by us earlier. It is shown that regardless of SPP the anion self-diffusion in model crystals without surface or artificially embedded defects goes on via exchange mechanism, rather than interstitial or vacancy mechanisms suggested by the previous works. The activation energy of exchange diffusion turned out to coincide with the anti-Frenkel defect formation energy calculated by the lattice statics. © 2012 Elsevier B.V. All rights reserved.en
dc.format.mimetypeapplication/pdfen
dc.language.isoenen
dc.sourceJournal of Nuclear Materialsen
dc.subjectDEFECT FORMATION ENERGIESen
dc.subjectDIFFUSION ACTIVATION ENERGYen
dc.subjectEMBEDDED DEFECTSen
dc.subjectEXCHANGE DIFFUSIONen
dc.subjectEXCHANGE MECHANISMen
dc.subjectGRAPHICS PROCESSORen
dc.subjectHIGH-PRECISIONen
dc.subjectLATTICE STATICSen
dc.subjectLOW TEMPERATURESen
dc.subjectMOLECULAR DYNAMICS SIMULATIONSen
dc.subjectOXYGEN ANIONen
dc.subjectPAIR INTERACTIONSen
dc.subjectPAIR POTENTIALen
dc.subjectSELF-DIFFUSIONen
dc.subjectSUPERIONIC TRANSITIONen
dc.subjectTEMPERATURE DEPENDENCEen
dc.subjectVACANCY MECHANISMSen
dc.subjectACTIVATION ENERGYen
dc.subjectAPPROXIMATION THEORYen
dc.subjectCRYSTAL DEFECTSen
dc.subjectIONSen
dc.subjectMOLECULAR DYNAMICSen
dc.subjectMOLECULAR MECHANICSen
dc.subjectSURFACE DEFECTSen
dc.subjectDIFFUSIONen
dc.titleHigh-precision molecular dynamics simulation of UO2-PuO 2: Anion self-diffusion in UO2en
dc.typeArticleen
dc.typeinfo:eu-repo/semantics/publishedVersionen
dc.typeinfo:eu-repo/semantics/articleen
dc.identifier.doi10.1016/j.jnucmat.2012.08.033-
dc.identifier.scopus84867895212-
local.affiliationUral Federal University, Mira Street 19, 620002 Yekaterinburg, Russian Federationen
local.contributor.employeeПоташников Святослав Игоревичru
local.contributor.employeeБоярченков Антон Сергеевичru
local.contributor.employeeНекрасов Кирилл Александровичru
local.contributor.employeeКупряжкин Анатолий Яковлевичru
local.description.firstpage215-
local.description.lastpage226-
local.issue1-3-
local.volume433-
dc.identifier.wos000316153800029-
local.contributor.departmentФизико-технологический институтru
local.identifier.pure895948-
local.identifier.eid2-s2.0-84867895212-
local.identifier.wosWOS:000316153800029-
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