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dc.contributor.authorConstant, TJ
dc.contributor.authorTollerton, CJ
dc.contributor.authorHendry, E
dc.contributor.authorChang, DE
dc.date.accessioned2018-01-25T15:19:13Z
dc.date.issued2016-05-05
dc.description.abstractIt has recently been demonstrated that difference frequency mixing (DFM) can generate surface plasmons in graphene [1]. Here, we present detailed calculations comparing the contributions to this effect from substrate and from graphene nonlinearities. Our calculations show that the substrate (quartz) nonlinearity gives rise to a surface plasmon intensity that is around twelve orders of magnitude smaller than that arising from the intrinsic graphene response. This surprisingly efficient intrinsic process, given the centrosymmetric structure of graphene, arises almost entirely due to non-local contributions to the second order optical nonlinearity of graphene.en_GB
dc.identifier.urihttp://hdl.handle.net/10871/31186
dc.language.isoenen_GB
dc.publisherarXiv.orgen_GB
dc.relation.urlhttp://arxiv.org/abs/1605.01542v1en_GB
dc.titleThe Roles of Substrate vs Nonlocal Optical Nonlinearities in the Excitation of Surface Plasmons in Grapheneen_GB
dc.typeArticleen_GB
dc.date.available2018-01-25T15:19:13Z
dc.identifier.journalarXiven_GB


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