Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/2511
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dc.contributorDepartment of Applied Physics-
dc.creatorLam, CH-
dc.date.accessioned2014-12-11T08:27:06Z-
dc.date.available2014-12-11T08:27:06Z-
dc.identifier.issn0021-8979-
dc.identifier.urihttp://hdl.handle.net/10397/2511-
dc.language.isoenen_US
dc.publisherAmerican Institute of Physicsen_US
dc.rights© 2010 American Institute of Physics. This article may be downloaded for personal use only. Any other use requires prior permission of the author and the American Institute of Physics. The following article appeared in C.H. Lam, J. Appl. Phys. 108, 064328 (2010) and may be found at http://link.aip.org/link/?jap/108/064328en_US
dc.subjectElasticityen_US
dc.subjectGe-Si alloysen_US
dc.subjectIsland structureen_US
dc.subjectMonte Carlo methodsen_US
dc.subjectNanofabricationen_US
dc.subjectSelf-assemblyen_US
dc.subjectSemiconductor growthen_US
dc.subjectSemiconductor quantum dotsen_US
dc.subjectSolid-state phase transformationsen_US
dc.subjectSurface energyen_US
dc.subjectSurface reconstructionen_US
dc.titleKinetic Monte Carlo simulation of shape transition of strained quantum dotsen_US
dc.typeJournal/Magazine Articleen_US
dc.identifier.spage1-
dc.identifier.epage8-
dc.identifier.volume108-
dc.identifier.issue6-
dc.identifier.doi10.1063/1.3483248-
dcterms.abstractThe pyramid-to-dome transition in Ge᙮Si₁₋᙮ on Si(100) initiated by step formation on pyramidal quantum dots is atomistically simulated using a multistate lattice model in two-dimensions incorporating effective surface reconstructions. Under quasiequilibrium growth conditions associated with low deposition rates, the transition occurs at island size nᴄ following (see article file for details of the abstract) independent of temperature and deposition rate. The shape transition is found to be an activated process. Results are explained by a theory based on simple forms of facet energies and elastic energies estimated using a shallow island approximation. An asymptotic scaling relation (see article file for details of the abstract) for x→0 applicable to d=2 or 3 dimensions is derived. The shape transition energy barrier can be dominated by the interface energy between steep and shallow facets.-
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationJournal of applied physics, 15 Sept. 2010, v. 108, no. 6, 064328, p.1-8-
dcterms.isPartOfJournal of applied physics-
dcterms.issued2010-09-15-
dc.identifier.isiWOS:000282646400151-
dc.identifier.scopus2-s2.0-77957728548-
dc.identifier.eissn1089-7550-
dc.identifier.rosgroupidr54026-
dc.description.ros2010-2011 > Academic research: refereed > Publication in refereed journal-
dc.description.oaVersion of Recorden_US
dc.identifier.FolderNumberOA_IR/PIRAen_US
dc.description.pubStatusPublisheden_US
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