Emergence of photoswitchable states in a graphene-azobenzene-Au platform

Abstract

The perfect transmission of charge carriers through potential barriers in graphene (Klein tunneling) is a direct consequence of the Dirac equation that governs the low-energy carrier dynamics. As a result, localized states do not exist in unpatterned graphene, but quasi-bound states \emph{can} occur for potentials with closed integrable dynamics. Here, we report the observation of resonance states in photo-switchable self-assembled molecular(SAM)-graphene hybrid. Conductive AFM measurements performed at room temperature reveal strong current resonances, the strength of which can be reversibly gated \textit{on-} and \textit{off-} by optically switching the molecular conformation of the mSAM. Comparisons of the voltage separation between current resonances ($\sim 70$--$120$ mV) with solutions of the Dirac equation indicate that the radius of the gating potential is $\sim 7\pm 2$ nm with a strength $\ge 0.5$ eV. Our results and methods might provide a route toward \emph{optically programmable} carrier dynamics and transport in graphene nano-materials.

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Cited by in corpus (6)

• Bielectron vortices in two-dimensional Dirac semimetals
• Optimal traps in graphene
• Conductance Switching of Azobenzene-Based Self-Assembled Monolayers on Cobalt Probed by UHV Conductive-AFM
• Minimal Geometry for Valley Filtering in Graphene
• Enhancement of thermoelectric figure of merit in zigzag graphene nanoribbons with periodic edge vacancies
• Electron Scattering in 2D Semiconductors: Contrasting Dirac and Schrödinger Behavior