High-capacity hydrogen storage by metallized graphene

buir.contributor.authorÇıracı, Salim
buir.contributor.orcidÇıracı, Salim|0000-0001-8023-9860
dc.citation.epage043123-3en_US
dc.citation.issueNumber4en_US
dc.citation.spage043123-1en_US
dc.citation.volumeNumber93en_US
dc.contributor.authorAtaca, C.en_US
dc.contributor.authorAktürk, E.en_US
dc.contributor.authorÇıracı, Salimen_US
dc.contributor.authorUstunel H.en_US
dc.date.accessioned2016-02-08T10:08:05Z
dc.date.available2016-02-08T10:08:05Z
dc.date.issued2008en_US
dc.departmentDepartment of Physicsen_US
dc.description.abstractFirst-principles plane wave calculations predict that Li can be adsorbed on graphene forming a uniform and stable coverage on both sides. A significant part of the electronic charge of the Li 2s orbital is donated to graphene and is accommodated by its distorted π* -bands. As a result, semimetallic graphene and semiconducting graphene ribbons change into good metals. It is even more remarkable that Li covered graphene can serve as a high-capacity hydrogen storage medium with each adsorbed Li absorbing up to four H2 molecules amounting to a gravimetric density of 12.8 wt %.en_US
dc.identifier.doi10.1063/1.2963976en_US
dc.identifier.issn1077-3118
dc.identifier.urihttp://hdl.handle.net/11693/23034
dc.language.isoEnglishen_US
dc.publisherAIP Publishingen_US
dc.relation.isversionofhttp://dx.doi.org/10.1063/1.2963976en_US
dc.source.titleApplied Physics Lettersen_US
dc.subjectHydrogenen_US
dc.subjectLithiumen_US
dc.subjectMetalsen_US
dc.subjectNonmetalsen_US
dc.subjectElectronic chargesen_US
dc.subjectFirst-principlesen_US
dc.subjectGrapheneen_US
dc.subjectGravimetric densityen_US
dc.subjectHigh-capacityen_US
dc.subjectHydrogen storage mediumen_US
dc.subjectPlane wave calculationsen_US
dc.subjectHydrogen storageen_US
dc.titleHigh-capacity hydrogen storage by metallized grapheneen_US
dc.typeArticleen_US

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