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dc.contributor.authorLiang, Z.en
dc.contributor.authorZhang, X.en
dc.contributor.authorWang, Y.en
dc.contributor.authorLv, S.en
dc.contributor.authorAlexandrov, D. V.en
dc.contributor.authorLiang, H.en
dc.contributor.authorYang, Y.en
dc.date.accessioned2025-02-25T11:02:21Z-
dc.date.available2025-02-25T11:02:21Z-
dc.date.issued2024-
dc.identifier.citationLiang, Z., Zhang, X., Wang, Y., Lv, S., Alexandrov, D. V., Liang, H., & Yang, Y. (2024). A Comparative Computational Study of the Solidification Kinetic Coefficients for the Soft-Sphere BCC-Melt and the FCC-Melt Interfaces. Crystals, 14(4), [292]. https://doi.org/10.3390/cryst14040292apa_pure
dc.identifier.issn2073-4352-
dc.identifier.otherFinal2
dc.identifier.otherAll Open Access; Gold Open Access3
dc.identifier.otherhttps://www.scopus.com/inward/record.uri?eid=2-s2.0-85191361203&doi=10.3390%2fcryst14040292&partnerID=40&md5=38c48093eedbbc4e496603d0a186aa601
dc.identifier.otherhttps://www.mdpi.com/2073-4352/14/4/292/pdf?version=1711088899pdf
dc.identifier.urihttp://elar.urfu.ru/handle/10995/141712-
dc.description.abstractUsing the non-equilibrium molecular dynamics (NEMD) simulations and the time-dependent Ginzburg–Landau (TDGL) theory for solidification kinetics, we study the crystal-melt interface (CMI) kinetic coefficients for both the soft-sphere (SS) BCC-melt and the FCC-melt interfaces, modeled with the inverse-power repulsive potential ((Formula presented.)). The collective dynamics of the interfacial liquids at four equilibrium CMIs are calculated and employed to eliminate the discrepancy between the predictions of the kinetic coefficient using the NEMD simulations and the TDGL solidification theory. The speedup of the two modes of the interfacial liquid collective dynamics (at wavenumbers equal to the principal and the secondary reciprocal lattice vector of the grown crystal) at the equilibrium FCC CMI is observed. The calculated local collective dynamics of the SS BCC CMIs are compared with the previously reported data for the BCC Fe CMIs, validating a hypothesis proposed recently that the density relaxation times of the interfacial liquids at the CMIs are anisotropic and material dependent. With the insights provided by the improved application of the TDGL solidification theory, an attempt has been made to interpret the variation physics of the crystal-structure dependence of the solidification kinetic coefficient. © 2024 by the authors.en
dc.description.sponsorshipNational Natural Science Foundation of China, NSFC, (11874147); National Natural Science Foundation of China, NSFC; Natural Science Foundation of Shanghai Municipality, (23ZR1420200); Natural Science Foundation of Shanghai Municipalityen
dc.description.sponsorshipThis research was funded by Yang Yang of the Chinese National Science Foundation (Grant No. 11874147), the Natural Science Foundation of Shanghai (Grant No. 23ZR1420200).en
dc.format.mimetypeapplication/pdfen
dc.language.isoenen
dc.publisherMultidisciplinary Digital Publishing Institute (MDPI)en
dc.rightsinfo:eu-repo/semantics/openAccessen
dc.rightscc-byother
dc.sourceCrystals2
dc.sourceCrystalsen
dc.subjectKINETIC COEFFICIENTen
dc.subjectNON-EQUILIBRIUM MOLECULAR DYNAMICSen
dc.subjectSOLIDIFICATION KINETICSen
dc.subjectTIME-DEPENDENT GINZBURG–LANDAU THEORYen
dc.titleA Comparative Computational Study of the Solidification Kinetic Coefficients for the Soft-Sphere BCC-Melt and the FCC-Melt Interfacesen
dc.typeArticleen
dc.typeinfo:eu-repo/semantics/articleen
dc.typeinfo:eu-repo/semantics/publishedVersionen
dc.identifier.doi10.3390/cryst14040292-
dc.identifier.scopus85191361203-
local.contributor.employeeLiang Z., State Key Laboratory of Precision Spectroscopy, School of Physics and Electronic Science, East China Normal University, Shanghai, 200241, Chinaen
local.contributor.employeeZhang X., State Key Laboratory of Precision Spectroscopy, School of Physics and Electronic Science, East China Normal University, Shanghai, 200241, Chinaen
local.contributor.employeeWang Y., State Key Laboratory of Precision Spectroscopy, School of Physics and Electronic Science, East China Normal University, Shanghai, 200241, Chinaen
local.contributor.employeeLv S., State Key Laboratory of Precision Spectroscopy, School of Physics and Electronic Science, East China Normal University, Shanghai, 200241, Chinaen
local.contributor.employeeAlexandrov D.V., Laboratory of Multi-Scale Mathematical Modeling, Department of Theoretical and Mathematical Physics, Ural Federal University, Lenin Ave., 51, Ekaterinburg, 620000, Russian Federationen
local.contributor.employeeLiang H., State Key Laboratory of Precision Spectroscopy, School of Physics and Electronic Science, East China Normal University, Shanghai, 200241, Chinaen
local.contributor.employeeYang Y., State Key Laboratory of Precision Spectroscopy, School of Physics and Electronic Science, East China Normal University, Shanghai, 200241, Chinaen
local.issue4-
local.volume14-
dc.identifier.wos001220391000001-
local.contributor.departmentState Key Laboratory of Precision Spectroscopy, School of Physics and Electronic Science, East China Normal University, Shanghai, 200241, Chinaen
local.contributor.departmentLaboratory of Multi-Scale Mathematical Modeling, Department of Theoretical and Mathematical Physics, Ural Federal University, Lenin Ave., 51, Ekaterinburg, 620000, Russian Federationen
local.identifier.pure56691583-
local.description.order292
local.identifier.eid2-s2.0-85191361203-
local.fund.rsfNational Natural Science Foundation of China, NSFC, (11874147); National Natural Science Foundation of China, NSFC; Natural Science Foundation of Shanghai Municipality, (23ZR1420200); Natural Science Foundation of Shanghai Municipality
local.fund.rsfThis research was funded by Yang Yang of the Chinese National Science Foundation (Grant No. 11874147), the Natural Science Foundation of Shanghai (Grant No. 23ZR1420200).
local.identifier.wosWOS:001220391000001-
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