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dc.contributor.authorJansing, Christine
dc.contributor.authorMertins, Hans-Christoph
dc.contributor.authorGilbert, Markus C.
dc.contributor.authorTimmers, Heiko
dc.contributor.authorChoi, Choi, Suk-Ho
dc.contributor.authorGaupp, Andreas
dc.contributor.authorKrivenkov, Maxim
dc.contributor.authorVarykhalov, Andrei
dc.contributor.authorRader, Oliver
dc.contributor.authorLegut, Dominik
dc.contributor.authorOppeneer, Peter M.
dc.date.accessioned2016-09-08T07:17:49Z
dc.date.available2016-09-08T07:17:49Z
dc.date.issued2016
dc.identifier.citationPhysical Review B. 2016, vol. 94, issue 4, art. no. 045422.cs
dc.identifier.issn2469-9950
dc.identifier.issn2469-9969
dc.identifier.urihttp://hdl.handle.net/10084/112010
dc.description.abstractThe existence of natural birefringence in x-ray reflection on graphene is demonstrated at energies spanning the carbon 1s absorption edge. This new x-ray effect has been discovered with precision measurements of the polarization-plane rotation and the polarization-ellipticity changes that occur upon reflection of linearly polarized synchrotron radiation on monolayer graphene. Extraordinarily large polarization-plane rotations of up to 30∘, accompanied by a change from linearly to circularly polarized radiation have been measured for graphene on copper. Graphene on single crystalline cobalt, grown on tungsten, exhibits rotation values of up to 17∘. Both graphene systems show resonantly enhanced effects at the π∗ and σ∗ energies. The results are referenced against those obtained for polycrystalline carbon and highly oriented pyrolytic graphite (HOPG), respectively. As expected, polycrystalline carbon shows negligible rotation, whereas a huge maximum rotation of 140∘ has been observed for HOPG that may be considered a graphene multilayer system. HOPG is found to exhibit such large rotation values over a broad energy range, even well beyond the π∗ resonance energy due to the contributions of numerous graphene layers. To explain the origin of the observed natural birefringence of graphene, the Stokes parameters as well as the x-ray natural linear dichroism in reflection have been determined. It is shown that the birefringence directly results from the optical anisotropy related to the orthogonal alignment of π∗ and σ∗ bonds in the graphene layer. Our polarization analysis reveals a strong bonding of graphene on Co with a reduced σ∗ excitation energy and a strong tilt of 50% of the p z orbitals towards diagonal orientation. In contrast, graphene on Cu is weakly bound with an orthogonal orientation of the p z orbitals. Exhibiting such a large natural birefringence that can be controlled through substrate choice, and because of excellent heat conductivity, graphene materials have a potential to be used as tunable x-ray phase shifting λ/4 or λ/2 plates in the design of future high-intensity light sources.cs
dc.language.isoencs
dc.publisherAmerican Physical Societycs
dc.relation.ispartofseriesPhysical Review Bcs
dc.relation.urihttp://dx.doi.org/10.1103/PhysRevB.94.045422cs
dc.rights©2016 American Physical Societycs
dc.titleX-ray natural birefringence in reflection from graphenecs
dc.typearticlecs
dc.identifier.doi10.1103/PhysRevB.94.045422
dc.type.statusPeer-reviewedcs
dc.description.sourceWeb of Sciencecs
dc.description.volume94cs
dc.description.issue4cs
dc.description.firstpageart. no. 045422cs
dc.identifier.wos000379651000006


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