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dc.contributor.authorLekka, C. E.en
dc.contributor.authorEvangelakis, G. A.en
dc.date.accessioned2015-11-24T17:33:21Z-
dc.date.available2015-11-24T17:33:21Z-
dc.identifier.issn0254-0584-
dc.identifier.urihttps://olympias.lib.uoi.gr/jspui/handle/123456789/13849-
dc.rightsDefault Licence-
dc.subjectalloysen
dc.subjectphonons in crystal latticesen
dc.subjectadsorbate vibrationsen
dc.subjectcomputational modelingen
dc.subjectsimulationsen
dc.subjectelectronic-structureen
dc.subjectstructural-propertiesen
dc.subjectdisordered ni3alen
dc.subjectatomic-structureen
dc.subjectalloy surfacesen
dc.subjectvibrational entropyen
dc.subjectrippled relaxationen
dc.subjectnial(110) surfaceen
dc.subjectordered alloysen
dc.subjectfermi-surfaceen
dc.titleDynamical properties of the Ni3Al low index surfaces with and without Ni or Al adatoms from molecular dynamics simulationsen
heal.typejournalArticle-
heal.type.enJournal articleen
heal.type.elΆρθρο Περιοδικούel
heal.identifier.primaryDOI 10.1016/j.matchemphys.2007.02.082-
heal.identifier.secondary<Go to ISI>://000247715300051-
heal.languageen-
heal.accesscampus-
heal.recordProviderΠανεπιστήμιο Ιωαννίνων. Σχολή Θετικών Επιστημών. Τμήμα Μηχανικών Επιστήμης Υλικώνel
heal.publicationDate2007-
heal.abstractWe present molecular dynamics simulation results on the vibrational properties of the Ni3Al low index surfaces with and without Ni/Al adatoms. We found that the mean square displacements of both surface atoms and adatoms depend linearly upon temperature, the adatoms on the (1 1 0) face exhibiting vibrational amplitudes twice as large as on the other two surfaces. In addition, we found that all surfaces studied are expanded and rumpled, the rippling effect being more pronounced in the case of the (0 0 1) face with the Al atoms occupying the topmost position. In the cases of the (1 1 0) and the (1 1 1) surfaces the rippling is visible at several atomic layers beneath the surface. The adatoms are found to be contracted at ambient conditions, an effect that is significant when deposited on the (1 1 0) face, attaining the value of -10%. Moreover, from the calculated phonon density of states (DOS) and phonon spectral densities at room temperature, we found that the presence of surfaces modifies the bulk phonon DOS, exhibiting new modes some of which are located in the bulk phonon gap. The present results are in line with available experimental and theoretical results. (c) 2007 Elsevier B.V. All rights reserved.en
heal.publisherElsevieren
heal.journalNameMaterials Chemistry and Physicsen
heal.journalTypepeer reviewed-
heal.fullTextAvailabilityTRUE-
Appears in Collections:Άρθρα σε επιστημονικά περιοδικά ( Ανοικτά)

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