Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/4992
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dc.contributorInstitute of Textiles and Clothing-
dc.creatorWang, Sen_US
dc.creatorZhu, Len_US
dc.creatorChen, Qen_US
dc.creatorWang, Jen_US
dc.creatorDing, Fen_US
dc.date.accessioned2014-12-11T08:24:58Z-
dc.date.available2014-12-11T08:24:58Z-
dc.identifier.issn0021-8979en_US
dc.identifier.urihttp://hdl.handle.net/10397/4992-
dc.language.isoenen_US
dc.publisherAmerican Institute of Physicsen_US
dc.rights© 2011 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 S. Wang et al., J. Appl. Phys. 109, 053516 (2011) and may be found at http://link.aip.org/link/?jap/109/053516.en_US
dc.subjectDensity functional theoryen_US
dc.subjectElemental semiconductorsen_US
dc.subjectEnergy gapen_US
dc.subjectHydrogenen_US
dc.subjectSemiconductor thin filmsen_US
dc.subjectSiliconen_US
dc.titleStability and electronic structure of hydrogen passivated few atomic layer silicon films : a theoretical explorationen_US
dc.typeJournal/Magazine Articleen_US
dc.identifier.spage1en_US
dc.identifier.epage5en_US
dc.identifier.volume109en_US
dc.identifier.issue5en_US
dc.identifier.doi10.1063/1.3553838en_US
dcterms.abstractThe stability, electronic, and optical properties of two dimensional hydrogenated few atomic layer silicon (H-FLSi) are systematically studied with density functional theory calculations. The formation energy of H-FLSi decreases with increasing layer thickness and approaches zero at the thickness of double layer, suggesting that this material is energetically favorable and thus its experimentally synthesizing is feasible. Its bandgap decreases with the increase of the thickness and eventually approaches the value of bulk silicon. More interestingly, the bandgap of hydrogenated silicon films can be tuned by external electric field and even becomes metal. Importantly, the light absorption threshold and absorption peak of the H-Si mono- and bilayer locate in different energy regions and both move toward higher energy region as compared with those of the bulk silicon.-
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationJournal of applied physics, 1 Mar. 2011, v. 109, no. 5, 053516, p. 1-5en_US
dcterms.isPartOfJournal of applied physicsen_US
dcterms.issued2011-03-01-
dc.identifier.isiWOS:000288387900039-
dc.identifier.scopus2-s2.0-79953000521-
dc.identifier.eissn1089-7550en_US
dc.identifier.rosgroupidr51862-
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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