Using combined "LDA+ image potential" calculations we show that below the vacuum level a single graphene layer possesses a double Rydberg series of even ͑n + ͒ and odd ͑n − ͒ symmetry image-potential states and argue that the widely discussed interlayer band in graphite is a consequence of the intersheet hybridization of the first even image-potential state. In light of the present results, the unoccupied electronic states with nearly-free-electron properties in carbon nanotubes, fullerenes, and fullerites can be understood to originate from the image-potential states of graphene.
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