Please use this identifier to cite or link to this item: http://dspace.utpl.edu.ec/jspui/handle/123456789/18812
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dc.contributor.authorStashans, A.es_ES
dc.contributor.authorGomez, C.es_ES
dc.contributor.authorVillamagua Conza, L.es_ES
dc.contributor.authorCarini, M.es_ES
dc.date.accessioned2017-06-16T22:02:25Z-
dc.date.available2017-06-16T22:02:25Z-
dc.date.issued2016-05-06es_ES
dc.identifier10.1007/s11587-016-0278-8es_ES
dc.identifier.isbn355038es_ES
dc.identifier.other10.1007/s11587-016-0278-8es_ES
dc.identifier.urihttp://dspace.utpl.edu.ec/handle/123456789/18812-
dc.description.abstractBased on the density functional theory approach we explore the chances endured by energy gap (EG) of semiconducting (armchair) graphene nanoribbons (AGNRs) when Stone-Wales (SW) defects are placed inside their lattices. Our results show that the AGNRs, which belong to the (Formula presented.) family experience an increase in their EG value. On the other hand, those belonging to 3m and (Formula presented.) families experience decrease in their EG. The maximum observed EG for pristine and distorted ribbons were (Formula presented.)2.6 and (Formula presented.)1.6 eV, respectively. Our results can be useful to understand the semiconducting properties of wider graphene nanoribbons which are already available experimentally.es_ES
dc.languageIngléses_ES
dc.subjectDensity functional theoryes_ES
dc.titleBand gap engineering of graphene through quantum confinement and edge distortionses_ES
dc.typeArticlees_ES
dc.publisherRicerche di Matematicaes_ES
Appears in Collections:Artículos de revistas Científicas



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