Structure of aluminum atomic chains

buir.contributor.authorÇıracı, Salim
buir.contributor.orcidÇıracı, Salim|0000-0001-8023-9860
dc.citation.epage195420-6en_US
dc.citation.issueNumber19en_US
dc.citation.spage195420-1en_US
dc.citation.volumeNumber64en_US
dc.contributor.authorSen, P.en_US
dc.contributor.authorÇıracı, Salimen_US
dc.contributor.authorBuldum, A.en_US
dc.contributor.authorBatra, I. P.en_US
dc.date.accessioned2016-02-08T10:34:22Z
dc.date.available2016-02-08T10:34:22Z
dc.date.issued2001en_US
dc.departmentDepartment of Physicsen_US
dc.description.abstractFirst-principles density-functional calculations reveal that aluminum can form planar chains in zigzag and ladder structures. The most stable one has equilateral triangular geometry with four nearest neighbors; the other stable zigzag structure has wide bond angle and allows for two nearest neighbors. An intermediary structure has the ladder geometry and is formed by two strands. While all these planar geometries are more favored energetically than the linear chain, the binding becomes even stronger in nonplanar geometries. We found that by going from bulk to a chain the character of bonding changes and acquires directionality. The conductance of zigzag and linear chains is 4e2/h under ideal ballistic conditions.en_US
dc.description.provenanceMade available in DSpace on 2016-02-08T10:34:22Z (GMT). No. of bitstreams: 1 bilkent-research-paper.pdf: 70227 bytes, checksum: 26e812c6f5156f83f0e77b261a471b5a (MD5) Previous issue date: 2001en
dc.identifier.issn0163-1829
dc.identifier.urihttp://hdl.handle.net/11693/24788
dc.language.isoEnglishen_US
dc.publisherAmerican Physical Societyen_US
dc.source.titlePhysical Review B - Condensed Matter and Materials Physicsen_US
dc.subjectAluminumen_US
dc.subjectCalculationen_US
dc.subjectChemical analysisen_US
dc.subjectChemical structureen_US
dc.subjectConductanceen_US
dc.subjectDensityen_US
dc.subjectGeometryen_US
dc.titleStructure of aluminum atomic chainsen_US
dc.typeArticleen_US

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